WorldWideScience

Sample records for aupres du tevatron

  1. Mesure de la section efficace de production de paires de quarks top dans le canal μ + jets + τ + b-jet(s) + Energie transverse manquante auprès de l'expérience DØ du Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Jammes, Jerome [Blaise Pascal Univ., Aubiere (France)

    2011-09-09

    The purpose of high energy physics is to improve our knowledge about the fundamental structure of matter, in particular about particles that constitute the world. One of these is the top quark, that was discovered in 1995 by the CDF and D0 collaborations at the Tevatron protons-antiprotons collider. One of the primary aim of the Tevatron has been then the fine study of the top quark properties, in particular the top-antitop production cross section. Different analysis have been performed in the leptons (μ,e,τ) + jets, dileptons, and all hadronic channels to determine accurately the values of these parameters, and thus to test the validity of the Standard Model. The main goal of this thesis is to verify one of the theoretical predictions of the Standard Model of particle physics, the top-antitop production cross section, at the Tevatron collider.

  2. Finding the Higgs boson of the standard model in the channel ZH → e+e-b$\\bar{b}$ with the D0 detector at the Tevatron; Recherche du boson de Higgs du nideke standard dans le canal ZH → e+e-b$\\bar{b}$ avec le detecteur DØ aupres du Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Calpas, Betty Constante [Univ. of the Mediterranean, Marseille (France)

    2010-06-11

    The organization of this thesis consists of three main ideas: the first presents the theoretical framework and experimental, as well as objects used in the analysis and the second relates to the various work tasks of service that I performed on the calorimeter, and the third is the search for the Higgs boson in the channel ZH → e+e-b$\\bar{b}$. Thus, this thesis has the following structure: Chapter 1 is an introduction to the standard model of particle physics and the Higgs mechanism; Chapter 2 is an overview of the complex and the acceleration of the Tevatron at Fermilab DØ detector; Chapter 3 is an introduction to physical objects used in this thesis; Chapter 4 presents the study made on correcting the energy measured in the calorimeter; Chapter 5 describes the study of certification of electrons in the calorimeter; Chapter 6 describes the study of certification of electrons in the intercryostat region of calorimeter; Chapter 7 Detailed analysis on the search for Higgs production in the channel ZH → e+e-b$\\bar{b}$; and Chapter 8 presents the final results of the calculations of upper limits to the production cross section of the Higgs boson on a range of low masses.

  3. Search for the supersymmetric partner of bottom quark at DO at Tevatron. Studies on missing transverse energy; Recherche du partenaire supersymetrique du quark bottom au sein de l'experience DO aupres du TeVatron. Etudes sur l'energie transverse manquante

    Energy Technology Data Exchange (ETDEWEB)

    Calvet, S

    2007-09-15

    Supersymmetry, the extension of the Standard Model of particle physics, is searched for, by trying to observe the supersymmetric partner of the bottom quark (b-bar). This search is performed by using events with a final state comprising 2 coplanar b-quark jets and missing transverse energy and coming from a sample of 992 pb{sup -1} of data collected by the D0 detector at the Tevatron, the Fermilab pp-bar collider. The absence of an excess of events in comparison to Standard Model expectations leads to exclude sb masses up to 201 GeV and neutralino masses up to 94 GeV. The missing transverse energy has been studied carefully under 2 points of view, because of its fundamental role in this search. First, at the level of the trigger system which allows the online selection candidate events, and then during the process Z {yields} {nu}{nu} + jets that is an important background noise and in which the transverse momentum of Z turns into missing energy because of the no-detection of the neutrinos. (author)

  4. Top quark mass measurement in the dilepton channel during the D0 experiment at the Tevatron. Mesure de la masse du quark top dans les canaux di-leptoniques auprès de l’expérience D0 au Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Croc, Aurelien [Commissariat a l' Energie Atomique et aux Energies Alternatives (CEA) Saclay, Gif-sur-Yvette (France). IRFU

    2011-01-01

    The top quark is the heaviest standard model quark. Discovered in 1995 by the two Tevatron experiments it has atypical properties. In particular its time life is so short that it decays before hadronizing, so the top quark mass could be measured with a high precision. Data collected by the DØ experiment between 2002 and 2009, which represent an integrated luminosity of 5.4 fb⁻¹, are used to measure the top quark mass by using the matrix element method in the three dilepton channels: dielectron, electron--muon and dimuon. The measured mass, 174.0 ± 1.8 (stat.) ± 2.4 (syst.) GeV, is in a good agreement with other measurements and limited by the systematic uncertainties for the first time in these channels. In this thesis different approaches have been studied to improve the accuracy of this measurement: the use of b-quark jet identification in order to optimize the selection of top--anti-top events and a better determination of the main systematic uncertainties. A special attention has been paid to the Monte-Carlo simulation of muons in D0: the improved smearing procedure for the simulated muons, discussed in this thesis, will be used to increase the accuracy of the top properties measurements as well as the precision of many other D0 measurements.

  5. Recherche du boson de Higgs dans l'état final dimuonique et étude de l'asymétrie de production de la paire top antitop avec l'expérience DO auprès du Tevatron; Higgs boson search in the dimuonique final state and study of the top pair antitop production asymmetry with the DO experiment at the Tevatron.

    Energy Technology Data Exchange (ETDEWEB)

    Fauré, Alexandre [University of Paris-Sud, Orsay (France)

    2014-06-03

    Two high energy particle physics analyses are presented in this PhD report using events with two leptons oppositely charged and with missing transverse energy. These events are selected using 9.7 fb-1 of total pp collisions data collected with the DØ detector at the TeVatron at √s=1.96 TeV.The first analysis is the research of the Higgs boson decaying in the H→WW→μνμν channel. No significant excess above the background prediction is observed.Upper limits on Higgs boson production cross-section are computed in the standard model framework but also in the 4th generation of fermions and in the fermiophobic coupling to Higgs boson hypotheses. In order to validate the research methodology, the W boson pair production cross-section is measured.The second analysis is the measurement of the forward-backward asymmetry of the tt pair production. This is the first measurement in the dileptonic channel at DØ experiment. In this context, a new tt pair kinematic reconstruction is used (matrix element method) to give a raw measurement of the forward-backward asymmetry. Thanks to a dedicated calibration method, we give a final measurement of AFB=18.0 ± 6.0 (stat) ± 3.3 (syst).

  6. Search for the Higgs boson in the WH channel and production of Wbb-bar in 1.96 TeV pp-bar collisions in the D0 experiment at the Fermilab Tevatron; Recherche du boson de Higgs dans le canal WH et etude de la production Wbb-bar dans les collisions pp-bar a 1.96 TeV dans l'experience D0 aupres du Tevatron de Fermilab

    Energy Technology Data Exchange (ETDEWEB)

    Beauceron, St

    2004-05-15

    The introduction of the Higgs boson in the standard model provides a mechanism to explain the origin of the masses of the elementary particles. The Higgs boson has not yet been discovered but a lower limit on its mass has been set at 114.4 GeV at 95% confidence level by LEP experiments. The search for the Higgs boson has been pursued at the Tevatron, proton-antiproton collider, in the associated production channel WH with a Higgs mass lower than 135 GeV where the Higgs decay in bb-bar. The detector D0 is used to record the signals. For this analysis, the calorimeter and the tracker are the main sub-detector. The signals from the calorimeter have been studied through a calibration and a study on the noise level in order to improve the reconstruction of the objects. The missing transverse energy, the electrons and the jets are well identified objects so they can be used in our analysis W({yields} e{nu}) + jets. As D0 has a new tracker and solenoid system, information from this system allow us to tag jets when they are originating from a b-quark. The analysis of events W({yields} e{nu}) + 2*b-tag jets has been made on 174 pb{sup -1}. An upper limit of the cross section production of the process W({yields} e{nu})bb-bar has been derived at 20.3 pb at 95% confidence level. This process is the main irreducible background of the WH {yields} e{nu}bb-bar. In the second part of the analysis, the search for the Higgs boson has been done for different mass values between 105 GeV and 135 GeV. Upper Limits on cross section production times branching ratio have been set. For a Higgs mass of 115 GeV, the upper limit is set of 12.4 pb at 95% confidence limit. (author)

  7. Search for the supersymmetric partner of the top quark in the channel stop anti-stop {yields} e{sup {+-}} {mu}{sup {+-}} sneutrino anti-sneutrino b anti-b in D0 experiment at the Tevatron. Calibration of the D0 electromagnetic calorimeter; Recherche du partenaire supersymetrique du quark top dans le canal stop anti-stop {yields} e{sup {+-}} {mu}{sup {+-}} sneutrino anti-sneutrino b anti-b au sein de l'experience D0 aupres du TeVatron. Calibration du calorimetre electromagnetique de D0

    Energy Technology Data Exchange (ETDEWEB)

    Mendes, A

    2006-10-15

    Symmetry is one of the most natural extensions of the standard model. At low energy it may consist in the Minimal Supersymmetric Standard Model which is the framework chosen to perform the search of the stop with 350 pb{sup -1} of data collected by D0 during the run-IIa period of the Tevatron. We selected the events with an electron, a muon, missing transverse energy and non-isolated tracks, signature for the stop decay in 3 particles (stop {yields} bl sneutrino). Since no significant excess of signal is seen, the results are interpreted in terms of limit on the stop production cross-sections, in such a way that we extend the existing exclusion region in the parameter space (m(stop), m(sneutrino)) up to stop masses of 168 (140) GeV for sneutrino masses of 50 (94) GeV. Finally, because of the crucial role of the electromagnetic calorimeter, a fine calibration was performed using Z {yields} e{sup +}e{sup -} events, which improved significantly the energy resolution. (author)

  8. La visite du camp : missions sanitaires du cicr auprès des prisonniers de guerre français détenus en Allemagne

    OpenAIRE

    Delpal, Bernard

    2015-01-01

    C’est un pays accablé par la défaite militaire, la débâcle, l’exode, un armistice humiliant et l’occupation qui, au cours de l’été 1940, doit subir la capture de près de deux millions d’hommes et leur envoi en Allemagne. À la fin du mois d’octobre 1940, alors que le transport des prisonniers de guerre (pg) est presque achevé, la Croix-Rouge française presse le Comité international de la Croix-Rouge (cicr) d’intervenir auprès du Reich pour adoucir des conditions de détention jugées insupportab...

  9. The search for the Higgs at the Tevatron; La recherche du Higgs au Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Lucotte, A

    2004-07-01

    The Tevatron has undergone an impressive technical renovation program whose final aim is to reach an integrated luminosity of 15 fb{sup -1} per experiment. Both CDF and DO detectors have been upgraded in the fields of detection, triggering, track reconstruction and particle identification. In the framework of the standard model, theoretical studies show that for a luminosity of only 2 fb{sup -1} (that is the first step of the renovation program) CDF and DO could barely extend the domain already excluded by LEP for the existence of the Higgs boson. On the other hand for a luminosity of 15 fb{sup -1}, a standard Higgs boson could be excluded up to 180 GeV/c{sup 2} and discovered up to 125 GeV/c{sup 2}. Moreover, a 3*{sigma} result could be obtained in the decay channels H {yields} bb-bar and H {yields} W{sup +}W{sup -} up to 180 GeV/c{sup 2}. In the framework of the minimal supersymmetric standard model (MSSM), at least 20 fb{sup -1} are required for the discovery of the Higgs boson in the energy range: 80 {<=} m{sub A} {<=} 380 GeV/c{sup 2}. (A.C.)

  10. Participation du patient Marocain atteint du cancer au choix thérapeutique: résultat d'une enquête réalisée auprès de 272 patient

    OpenAIRE

    Boukir, Anwar; Azghari, Ilham; El Kabous, Mustapha; Jouid, Khalid; Boutayeb, Saber; El Ghissassi, Ibrahim; Mrabti, Hind; Errrihani, Hassan

    2015-01-01

    Introduction La décision médicale partagée ‘Shared decision making’ est un concept qui se développe depuis les années 1990. Il donne aux patients le soutien nécessaire pour exprimer leurs préférences et partager la décision médicale. Cette étude cherche à estimer le degré de participation du patient Marocain atteint de cancer au choix thérapeutique. Méthodes Cette enquête a été réalisée auprès de 272 malades sous chimiothérapie pour une pathologie cancéreuse sous forme d'un entretien verbal b...

  11. 1er mars 2017 - Signature du livre d'or, visite du tunnel du LHC au Point 5 et de la caverne expériementale de CMS par le Secrétaire d’Etat français aux Affaires européennes auprès du ministre des Affaires étrangères et du Développement international H. Désir.

    CERN Multimedia

    Bennett, Sophia Elizabeth

    2017-01-01

    Entourent le Secrétaire d'Etat pendant la signature du livre d'or: Le Préfet de l’Ain A. Cochet; le Directeur des accélérateurs et de la technologie F. Bordry; Ambassadeur, Représentant permanent de la France auprès de l’Office des Nations Unies à Genève et des Organisations internationales en Suisse E. Laurin; la Directrice générale du CERN F. Gianotti et la Directrice des relations internationales C. Warakaulle. Sont également présents: H. Bertrand, Maire de Saint-Genis-Pouilly; C. Bouvier, Maire de Cessy; G. Rousseau, Secrétaire Général de la sous-préfecture de Gex; Y. Mecibah, Directrice de Cabinet du Maire de Saint-Genis-Pouilly; F. Croquette, Ambassadeur pour les droits de l’homme, chargé de la dimension internationale de la Shoah, des spoliations et du devoir de mémoire; S. Bonbayl, Conseillère technique, Cabinet du Secrétaire d’Etat chargé des Affaires Européennes au MAEDI; F. Cormon-Veyssière, Sous-Directrice des droits de l’Homme et des Affaires humanitaires au MAEDI...

  12. Vivre à domicile, deux ans après un AVC : Etude auprès des patients et des aidants du Luxembourg.

    OpenAIRE

    Baumann, Michèle

    2012-01-01

    Au Luxembourg, une recherche pluridisciplinaire a été réalisée auprès de 797 personnes victimes d’un accident vasculaire cérébral (AVC). Une enquête nationale a été menée comportant un volet épidémiologique effectué par le CRP-Santé, qui a rassemblé des données médico-administratives et des données cliniques issues des dossiers d’hospitalisation, et un volet de sociologie médicale par l’Université qui a interrogé 94 patients vivant au domicile, deux après la survenue de l’AVC, et leurs 62 aid...

  13. Les troubles du langage inauguraux et démence : étude des troubles lexicaux auprès de 28 patients au stade débutant de la maladie d'Alzheimer

    Directory of Open Access Journals (Sweden)

    Thery Juliette

    2012-07-01

    Full Text Available Les troubles du langage font partie, avec les troubles de la mémoire, des premiers signes cliniques cognitifs de la maladie d’Alzheimer. Au début de la maladie, ces troubles essentiellement expressifs touchent surtout le lexique, les autres aspects du langage (phonologie, syntaxe restant préservés plus longtemps. Afin de mieux caractériser ces troubles du langage inauguraux, nous avons évalué ces troubles auprès de 28 sujets (12 hommes et 16 femmes, âgés de 52 à 90 ans (moyenne d’âge : 73 ans, présentant une maladie d’Alzheimer au stade débutant (MMS > ou = à 20, moyenne = 23,79. Aucun de ces sujets ne présentait de troubles auditifs ou visuels non corrigés ni de troubles gnosiques visuels. L’examen des troubles lexicaux a consisté en la passation de 3 épreuves (dénomination, désignation et appariement d’images permettant d’évaluer conjointement pour les mêmes 54 items (contrôlés en termes de fréquence, longueur et catégorie sémantique la production et la compréhension lexicale ainsi que le traitement sémantique non verbal. Les résultats à ces épreuves ont été analysés en fonction des scores et temps seuils établis auprès d’une population contrôle de 369 sujets. Les résultats montrent que 62% des sujets examinés présente des troubles de la production lexicale caractérisés par la présence de paraphasies lexicales sémantiques et visuo-s��mantiques, de circonlocutions et de dénominations vides et des délais dans les réponses, dans l’épreuve de dénomination d’images. Ces troubles expressifs s’accompagnent de troubles sémantiques dans la mesure 72% des sujets présentent des scores pathologiques à l’épreuve d’appariement sémantique et dans une moindre proportion, sont associés à des troubles de la compréhension lexicale (44% de scores pathologiques en désignation. Ces chiffres, plus élevés que ceux de la littérature, confortent l’hypothèse de troubles lexico

  14. Developpement de competences de resolution reflexive de problemes environnementaux aupres d'enseignants en formation du Botswana: Apport d'un modele pedagogique base sur une recherche-action participative

    Science.gov (United States)

    Gauthier, Benoit

    2000-10-01

    Cette etude s'interesse au developpement de competences de resolution de problemes environnementaux dans un contexte culturel africain. Pour y parvenir, elle elabore un modele pedagogique pouvant se situer dans le cadre theorique de la vision reflexive emergeant presentement en education relative a l'environnement (ERE). Provenant du champ d'etude de la systemique, la methodologie des systemes souples (MSS) s'avere compatible avec le cadre de la reflexivite qui est emergent. Un modele pedagogique preliminaire fut ainsi etabli en transposant et en adaptant plusieurs des principes et des constituantes de la MSS au domaine de l'ERE. Ce modele, s'appuyant sur une strategie de recherche-action, a ete ensuite mis a l'essai aupres d'enseignants du secondaire en formation au Botswana, dans le cadre de leurs activites parascolaires. Cette recherche-developpement de type participatif s'appuie sur une analyse qualitative. Durant sa mise a l'essai, le modele preliminaire a subi plusieurs modifications generees entre autres par les interactions entre les participants et le facilitateur; ces modifications suggerent fortement une prise en charge par les participants de la demarche d'investigation, condition essentielle pour le developpement de competences de resolution de problemes environnementaux. Durant la demarche de resolution du probleme, des competences relatives a l'acquisition de connaissances sur la situation investiguee et a l'action environnementale ont ete sollicitees de maniere repetee. Ceci ne semble pas avoir ete le cas pour les competences associees a la reflexion par les participants sur leurs propres perceptions (metacognition), sur celles des autres ou encore sur la nature de la connaissance (cognition epistemique). En ce qui a trait a la conception de chaque apprenant concernant le probleme environnemental etudie, les observations recueillies tout au long de la demarche suggerent, pour certains des participants, une complexification. Le modele resultant de l

  15. La matério-vigilance dans un Centre Hospitalo-Universitaire du Centre-Est tunisien: enquête auprès des médecins

    Science.gov (United States)

    Mahjoub, Mohamed; Jedidi, Maher; Masmoudi, Tasnim; Bouafia, Nabiha; Njah, Mansour

    2016-01-01

    Introduction Pour la meilleure gestion des risques en milieu hospitalier et l’amélioration de la qualité et la sécurité de nos soins, le CHU de Sousse (Tunisie), a mis en place, suite aux recommandations de l’ANCSEP (Agence Nationale de Contrôle Sanitaire et Environnementale des Produits) un système de matério-vigilance (MV). En Tunisie l’absence d’un cadre réglementaire organisant la MV est l’obstacle majeur à l’implication des soignants à ce système. L’objectif de cette étude est de déterminer les connaissances, attitudes et pratiques des médecins du CHU quant à la mise en place du système de MV. Méthodes Etude descriptive de type CAP (connaissances, attitudes et pratiques) transversale auprès de tous les médecins titulaires exerçant au CHU de Sousse (Tunisie) qui sont utilisateurs des dispositifs médicaux (DMs) lors de leur pratique d’activité de soin. Un questionnaire auto-administré, préétabli et pré-testé a été établi. Saisie et l’analysée des données par logiciel SPSS20.0. Résultats Le taux de réponse de 51,9 % (183/95), un manque des connaissances relatif à la MV a été rapporté. Plus de la moitié des répondants ne connaissent pas le correspondant local de son établissement et l’existence d’un formulaire standardisé de signalement. Concernant les attitudes, 89,5 % notifient l’intérêt de mise en place du système de MV et 37,5 % reconnaissent que le signalement doit émaner du soignant constatant l’incident. Pour les pratiques, la majorité confirment l’absence d’une gestion organisée de la maintenance des DMs dans leurs services. 90,5 % expriment leurs souhaits de recevoir une information mais peu d’entre eux expriment leurs désirs de suivre une formation (57,9 %). Conclusion Un manque d’information et de formation dans un domaine pourtant sensible et devant être lourdement réglementé est soulevé. La promulgation de textes réglementaires est nécessaire afin de promouvoir le

  16. Performances du calorimètre électromagnétique et recherche de nouveaux bosons de jauge dans le canal diélectron auprès du détecteur ATLAS

    CERN Document Server

    Laisne, Emmanuel; Trocme, B

    The Standard Model of particle physics has known a tremendous rise during the twentieth century. Built up from the early 1930s to the 1970s, this theory describing elementary particles and their interactions has now been intensively tested by LEP and Tevatron colliders. Besides its success, some questions remain and theories attempting to go beyond the Standard Model have emerged. Many of them are predicting the existence of a new gauge boson Z', which is supposed to be observable at the TeV scale. Data recorded by the LHC since autumn 2008 are a new opportunity to check the consistency of the Standard Model and to search for new physics evidence. Work that has been done by the ATLAS collaboration during the last four years has focused on understanding detector's behaviour and analysing the very first collected collisions. This thesis is reflecting these two aspects. The first part of this thesis describes the caracterisation of a pathology of the ATLAS liquid argon calorimeter electronics and the study of co...

  17. Search for Kaluza-Klein gravitons of the Randall-Sundrum model in the dimuon channel with the D0 detector at Tevatron; Etude de la production de graviton de Kaluza-Klein dans ses desintegrations en paires de muons dans le modele de Randall-Sundrum aupres de l'experience D0 au Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Lahrichi, N

    2004-07-01

    In this thesis we have put the first constraints on the fundamental parameters of the Randall-Sundrum model of extra dimensions, k/M{sub Pl} which is proportional to the coupling of the graviton to the standard model fields and M{sub G} which is the mass of the first excited state of the Kaluza-Klein graviton. The analysis performed on Monte Carlo sample of the signal allowed to find an error in the PYTHIA generator. The elaboration of an independent generator dedicated for this special analysis helped to find out and correct the error. The data sample used for the analysis covers the period running from november 2002 up to july 2003 taken by the D0 collaboration at Tevatron, which corresponds to an accumulated luminosity of 107,8 pb{sup -1}. The search for the graviton in the dimuon channel allowed to measure the Z production cross-section multiplied by the branching ratio in dimuons. (author)

  18. Recherche du virus BoHV-4 en cas d’avortement bovin en France : enquête auprès des laboratoires départementaux d’analyses vétérinaires

    OpenAIRE

    Chevanne, E.; Grimard, Bénédicte; Remy, Dominique

    2014-01-01

    Le BoHV-4 (Bovine HerpesVirus type 4) est un gammaherpèsvirus découvert en 1963. Cosmopolite, il infecte naturellement un large spectre d’hôtes dont les bovins domestiques. La séroprévalence individuelle du virus chez les bovins varie selon les études (5,9 % à 18 % ; Markine- Goriaynoff et al., 2003), mais il reste méconnu en France. Isolé à partir d’individus malades présentant une multitude de signes cliniques mais aussi d’individus sains, il semble préférentiellement engendrer des troubles...

  19. Search for squarks and gluinos in the D0 experiment of the Run-II-a at the Tevatron; Recherche des squarks et des gluinos dans l'experience D0 au Run-II-a du Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Verdier, P

    2007-11-15

    The D0 experiment is recording pp-bar collisions at a center-of-mass energy of 1.96 TeV since the beginning of the Run II-a of the Tevatron in 2001. The design of processor boards for the D0 level 2 trigger system is first presented. Those boards were installed in 2003, and they have been working perfectly since that date. Performances of missing transverse energy (/ ET ) reconstruction are then described. This quantity is important at hadron colliders especially for new particles searches. Finally, squarks and gluinos, supersymmetric partners of quarks and gluons, could be the most copiously produced supersymmetric particles at the Tevatron, if they are sufficiently light. Those particles were searched for in 0.96 fb{sup -1} of data recorded by D0 during the Run II-a. The final state consists of jets and missing transverse energy. The numbers of observed events are in good agreement with the Standard Model predictions. Lower mass limits at 95 % confidence level are obtained on the squark and gluino masses in the framework of the mSUGRA model. Contributions to other D0 data analyses are also shortly described. Those analyses are the search for first generation leptoquarks and the search for squarks in jets+{tau}(s)+E{sub T} events. The possibility to constrain a 'Little Higgs' model using the results of the jets+E{sub T} searches is then discussed. (author)

  20. Search for the Higgs Boson and for Anomalous Quartic Gauge Boson Couplings in the WW Channel with Dielectron Events with the D0 Experiment at the Tevatron; Recherche du boson de Higgs et de couplages de jauge quartiques anormaux dans le canal WW en électrons dans l'expérience D0 au Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Chapon, Emilien [Pierre and Marie Curie Univ., Paris (France)

    2013-01-01

    Le paysage de la physique des particules a subi des changements majeurs entre le début de cette thèse, en septembre 2010, et sa n en juin 2013. On peut notamment qualier l'année 2012 de date-clé dans l'histoire de la physique des particules. En 2012, une nouvelle particule a été découverte au LHC [1, 2], dont la majeure partie de la communauté s'accorde aujourd'hui à dire qu'il s'agit très probablement du boson de Higgs. Cet événement est intervenu peu après une sorte de passage de relais entre le Tevatron, arrêté le 30 septembre 2011, et le LHC, dont les toutes premières collisions sont intervenues le 23 novembre 2009.

  1. 29 August 2013 - J.-F. Jauslin, Directeur de l’Office fédéral de la culture (OFC) Ambassadeur suisse auprès de l’UNESCO et de l’OIF au 1er septembre 2013 Confédération suisse visite le centre visiteurs de l’expérience ATLAS ainsi que la caverne expérimentale d'ATLAS avec P. Jenny, ancien Porte-parole d'ATLAS. M. Bona, Conseiller du Directeur général pour les relations avec les Organisations internationales présent tout au long.

    CERN Multimedia

    Jean-Claude Gadmer

    2013-01-01

    29 August 2013 - J.-F. Jauslin, Directeur de l’Office fédéral de la culture (OFC) Ambassadeur suisse auprès de l’UNESCO et de l’OIF au 1er septembre 2013 Confédération suisse visite le centre visiteurs de l’expérience ATLAS ainsi que la caverne expérimentale d'ATLAS avec P. Jenny, ancien Porte-parole d'ATLAS. M. Bona, Conseiller du Directeur général pour les relations avec les Organisations internationales présent tout au long.

  2. Study of the signal H{sup 0}/A{sup 0} {yields} {tau}{mu} in hadron colliders and inter-calibration of the Ddiameter calorimeter with RUN 2 of Tevatron; Etude du signal H{sup 0}/A{sup 0} {yields} {tau}{mu} aux collisionneurs hadroniques et intercalibration du calorimetre de Ddiametre au RUN 2 du Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Delsart, P.A

    2003-10-01

    D0 is one of the 2 detectors settled on the Tevatron at Fermilab. This thesis has been made in collaboration with the 'theory' group and the D0 group of IPNL (nuclear physics institute of Lyon). Within the D0 group we have worked on the calibration of the detector's calorimeter: intercalibration. Using the fact that the physics is phi-symmetric in D0 we have created and applied statistical methods for a relative calibration of some phi-symmetric parts of the calorimeter. Work on particle physics concerned the two Higgs doublet model. In such models leptonic number violation is possible: we have simulated the H{sup 0}/A{sup 0} {yields} {tau}{mu} signal in order to study the discovery potential and the constraints on the coupling responsible for this decay. (author)

  3. Search for the scalar partner of the top quark and contribution to the improvement of the calorimetry of the experiment D zero for the phase 2 of Tevatron; Recherche du partenaire supersymetrique du quark top et contribution a l'amelioration de la calorimetrie de l'experience D zero pour la phase 2 du tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Olivier, B

    2001-04-01

    Supersymmetry could be the most natural extension of the Standard Model. In this thesis we present a new search for the sTop, the hypothetical scalar partner of the Top quark, that we performed in the framework of the Minimal Supersymmetric Standard Model (MSSM), using the Run I data of the DO experiment, which corresponds to an integrated luminosity of 108 pb{sup -1}. We selected events with one electron, one muon and missing transverse energy in the final state, which can be the decay product of pair of sTop quarks in 3 (t-tilde {yields} bl{nu}-tilde), or 4-body (t-tilde {yields} b{chi}-tilde{sub 1}{sup 0}l{nu}{sub l}). No signal is seen and the results are interpreted in terms of limits on the sTop production cross-section and exclusion regions in the parameter space (m{sub t}-tilde,m{sub {chi}}-tilde{sub 1{sup 0}}) or (m{sub t}-tilde,m{sub {nu}}-tilde). This new type of selection at the Tevatron for the search of the sTop allowed us to put stronger constraints than those previously published at LEP or at the Tevatron in the t-tilde {yields} bl{nu}-tilde channel, and the first limits ever set in the 4-body decay channel. For the 3-body channel, assuming that the sneutrino is the lightest supersymmetric particle (LSP), the excluded region at 95% confidence level extends up to a sTop mass of 142 (130) GeV if the sneutrino mass (m{sub {nu}}-tilde) is 43 (86) GeV. If the 4-body decay channel dominates, assuming that the neutralino is the LSP, the limit depends on the sneutrino mass. If it is light enough (m{sub {nu}}-tilde {approx}< 100 GeV) this limit reaches a sTop mass of 132 GeV for a neutralino mass of 60 GeV. In all searches for new particles, the calorimetry plays a crucial role from the experimental point of view. The expected increase in integrated luminosity in the Run II which started on the 1. of March 2001, and the detector upgrade which has been achieved over the last three years will allow to extend these exclusion domains or to discover the sTop. We

  4. Physics at the Tevatron

    Science.gov (United States)

    Field, R.

    2008-10-01

    The theme of the XXXIV International Meeting on Fundamental Physics on April 27, 2006 was "From HERA and the TEVATRON to the LHC". At that meeting I presented four lectures on "Physics at the Tevatron". This is a summary of two lectures on "Physics at the Tevatron: IMFP06 IMFP08" presented at the XXXVI International Meeting on Fundamental Physics held in Baeza, Spain on February 4-8, 2008. These two lectures are an attempt to highlight what we have learned at the Tevatron since my lectures in 2006. I will also look back at the "old days" of Feynman-Field collider phenomenology.

  5. 10 janvier 2014 - A. Kilani, Ambassadeur Représentant permanent de la Tunisie auprès de l'Office des Nations Unies à Genève et des institutions spécialisées en Suisse visite la caverne de l'expérience ATLAS avec P. Jenni, ancien porte-parole d'ATLAS; visite le tunnel du LHC au Point 1 avec J.M. Jiménez, Chef du Département Technologie et signe le livre d'or avec F. Bordry, Directeur des accélérateurs et de la technologie. P. Fassnacht, Bureau des Relations internationales, Conseiller pour la République tunisienne présent.

    CERN Multimedia

    Jean-Claude, Gadmer

    2014-01-01

    10 janvier 2014 - A. Kilani, Ambassadeur Représentant permanent de la Tunisie auprès de l'Office des Nations Unies à Genève et des institutions spécialisées en Suisse visite la caverne de l'expérience ATLAS avec P. Jenni, ancien porte-parole d'ATLAS; visite le tunnel du LHC au Point 1 avec J.M. Jiménez, Chef du Département Technologie et signe le livre d'or avec F. Bordry, Directeur des accélérateurs et de la technologie. P. Fassnacht, Bureau des Relations internationales, Conseiller pour la République tunisienne présent.

  6. 16 septembre 2015 - Signature du livre d'or par S. Exc. Mme Laurin, Ambassadeur de France auprès de l’Office des Nations Unies et des organisations internationales en Suisse avec le Directeur général du CERN R. Heuer, et de la Directrice générale élue 2016-2020 F. Gianotti.

    CERN Multimedia

    Brice, Maximilien

    2015-01-01

    Son Excellence Madame Elisabeth Laurin Ambassadeur Représentant permanent de la République française auprès de l’Office des Nations Unies et des organisations internationales en Suisse République française. Sont également présents: E. Göniger Voss, S. Péron, O. Martin, F. Bordry, A-S. Catherin, F. Eder.

  7. Celebrating the Tevatron legacy

    CERN Multimedia

    2012-01-01

    Fermilab hosted an exceptional event on 11 June: the Tevatron Impact symposium. More than 800 people attended to hear how the Tevatron advanced our understanding of fundamental physics.   A version of this "Director's Corner" by Pier Oddone first appeared in Fermilab Today on 12 June.   The development of accelerator technology for the Tevatron has influenced every subsequent major hadron accelerator. We heard reviews on the detector technologies and trigger systems developed with the Tevatron that are essential today for high-luminosity machines like the LHC. There were also talks on the superconducting-wire industry that made MRI magnets ubiquitous, and we discussed the major computational systems that use large farms of Linux-based commodity processors. Researchers who worked on the Tevatron also established multivariate analysis techniques that now allow us to squeeze the maximum information from complex data sets. One focus of the symposium was the ...

  8. Physics at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Field, Rick; /Florida U.

    2006-04-01

    The theme of the XXXIV International Meeting on Fundamental Physics held in El Escorial, Spain on April 2-7, 2006 was ''From HERA and the TEVATRON to the LHC''. This is a summary of the four lectures I presented on ''Physics at the Tevatron''. Heavy quark production and the production of photons, bosons, and jets at the Tevatron are discussed. Also, a detailed study at the ''underlying event'' at CDF is presented together with a discussion of PYTHIA 6.2 tunes. A look back at the ''old days'' of Feynman-Field collider phenomenology is included.

  9. Tevatron's complex collider cousins

    CERN Multimedia

    Fischer, W

    2004-01-01

    Letter referring to Schwarzschild's story "Disappointing performance and tight budgets confront Fermilab with tough decisions" and contesting that the Tevatron is not the most complex accelerator operating. They use the examples of CERN's SPS collider, HERA at DESY and the RHIC at Brookhaven (1/4 page)

  10. Optical stochastic cooling in Tevatron

    CERN Document Server

    Lebedev, V

    2012-01-01

    Intrabeam scattering is the major mechanism resulting in a growth of beam emittances and fast luminosity degradation in the Tevatron. As a result in the case of optimal collider operation only about 40% of antiprotons are used to the store end and the rest are discarded. Beam cooling is the only effective remedy to increase the particle burn rate and, consequently, the luminosity. Unfortunately neither electron nor stochastic cooling can be effective at the Tevatron energy and bunch density. Thus the optical stochastic cooling (OSC) is the only promising technology capable to cool the Tevatron beam. Possible ways of such cooling implementation in the Tevatron and advances in the OSC cooling theory are discussed in this paper. The technique looks promising and potentially can double the average Tevatron luminosity without increasing its peak value and the antiproton production.

  11. Tevatron extraction microcomputer

    Energy Technology Data Exchange (ETDEWEB)

    Chapman, L.; Finley, D.A.; Harrison, M.; Merz, W.

    1985-06-01

    Extraction in the Fermilab Tevatron is controlled by a multi-processor Multibus microcomputer system called QXR (Quad eXtraction Regulator). QXR monitors several analog beam signals and controls three sets of power supplies: the ''bucker'' and ''pulse'' magnets at a rate of 5760 Hz, and the ''QXR'' magnets at 720 Hz. QXR supports multiple slow spills (up to a total of 35 seconds) with multiple fast pulses intermixed. It linearizes the slow spill and bucks out the high frequency components. Fast extraction is done by outputting a variable pulse waveform. Closed loop learning techniques are used to improve performance from cycle to cycle for both slow and fast extraction. The system is connected to the Tevatron clock system so that it can track the machine cycle. QXR is also connected to the rest of the Fermilab control system, ACNET. Through ACNET, human operators and central computers can monitor and control extraction through communications with QXR. The controls hardware and software both employ some standard and some specialized components. This paper gives an overview of QXR as a control system; another paper summarizes performance.

  12. Etude exploratoire des conceptions de la circulation sanguine aupres d'eleves de l'ordre collegial

    Science.gov (United States)

    Robitaille, Jean-Marc

    Il existe peu d'etudes sur les conceptions touchant les domaines de la biologie, notamment sur les conceptions de la circulation sanguine Nous avons observe egalement l'absence de recherche menee aupres d'eleves de l'ordre collegial sur cette question. Nous avons voulu combler une lacune en menant une recherche sur les conceptions de la circulation sanguine aupres d'eleves de l'ordre collegial. Pour mener cette recherche nous nous sommes inspires d'une methode developpee par Treagust (1988). Le premier niveau de formulation didactique etablit l'architecture du systeme et la fonction nutritive de la circulation. Le second niveau de formulation didactique decrit et relie les parametres de la dynamique de la circulation et leur relation: Pression, Debit et Resistance. Le troisieme niveau de formulation didactique s'interesse au controle de la circulation du sang dans un contexte d'homeostasie qui implique la regulation de la pression arterielle. Nous avons construit un questionnaire en nous guidant sur les niveaux de formulation didactique et l'analyse des entrevues menees aupres de dix-huit eleves, representatifs de la population cible. Ce questionnaire fut administre a un echantillon de 2300 eleves disperses dans six colleges de la region de Montreal. Notre echantillon comprend des eleves inscrits a des programmes de l'ordre collegial en Sciences de la nature et en Techniques de la sante et qui n'ont pas suivi le cours sur la circulation sanguine. Notre analyse des reponses des eleves de notre echantillon aux questions sur le premier niveau de formulation didactique revele que la majorite des eleves considerent que le systeme circulatoire relie les organes les uns aux autres dans un circuit en serie. Notre analyse revele egalement que la majorite des eleves estiment que les nutriments sont extraits du sang par les organes selon un processus de selection base sur les besoins determines par la fonction de l'organe. Ces besoins sont differents selon les organes qui ne

  13. The issue of mass generation: the search for the Higgs boson in the D0 experiment at the proton-antiproton collider of Fermilab and the measurement of neutrino oscillation with OPERA; L'enigme de la generation des masses: la recherche du higgs dans l'experience D0 aupres du collisionneur proton-antiproton de Fermilab et la mesure des oscillations neutrinos a OPERA

    Energy Technology Data Exchange (ETDEWEB)

    Lucotte, A

    2004-09-01

    The first part is dedicated to the theoretical aspects of the mechanism of mass generation in the standard model. The implications of this mechanism in the experimental field concerning the Higgs boson search and neutrinos are detailed. The second part presents the D0 experiment at the Tevatron (Fermilab) and describes in a detailed way the forward pre-shower (FPS) that is a sub-detector of D0 whose aim is to identify the electrons. FPS has required a specific triggering system linked to a data acquisition line. The third part is devoted to the Opera experiment that is planned to operate in 2006. The purpose of this experiment is to confirm the oscillations of muon neutrinos and tau neutrinos through the direct detection of a tau lepton in the pure beam of muon neutrinos produced in CERN. The author describes his contribution to the design and testing of the front-end read electronics of the Opera scintillator tracker. (A.C.)

  14. Recent results from the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Vellidis, Costas; Bravina, L.; Foka, Y.; Kabana, S.

    2015-01-01

    The Tevatron p$\\bar{p}$ collider was shut down in 2011, after 10 years of high performance operation at a center-of-mass energy √s = 1.96 TeV in Run II. The two experiments, CDF and DZero, continue to analyze the collected data, aiming to extract all possible information regarding studies of the standard model and searches for new physics. A short review of some of the recent measurements at the Tevatron, and of the impact of the Tevatron program to high energy physics, is presented.

  15. Tevatron instrumentation: boosting collider performance

    Energy Technology Data Exchange (ETDEWEB)

    Shiltsev, Vladimir; Jansson, Andreas; Moore, Ronald; /Fermilab

    2006-05-01

    The Tevatron in Collider Run II (2001-present) is operating with six times more bunches, many times higher beam intensities and luminosities than in Run I (1992-1995). Beam diagnostics were crucial for the machine start-up and the never-ending luminosity upgrade campaign. We present the overall picture of the Tevatron diagnostics development for Run II, outline machine needs for new instrumentation, present several notable examples that led to Tevatron performance improvements, and discuss the lessons for the next big machines--LHC and ILC.

  16. Tevatron Higgs results

    CERN Document Server

    Tuchming, Boris

    2013-01-01

    We present the combination of searches for the Standard Model Higgs boson, using up to 10 \\invfb\\ of $p\\bar p$ collisions at $\\sqrts$=1.96 TeV collected with the CDF and \\dzero\\ detectors at the Fermilab Tevatron collider. The major contributing channels are optimized for the main production modes, the associated production with a vector boson ($VH$, with $V=W,Z$), the vector boson fusion, and the gluon-gluon fusion, and the different decay modes $H\\to b\\bar b$, $H\\to\\tau^+\\tau^-$, $H\\to W^+W^-$, and $H\\to \\gamma\\gamma$. A significant excess of events is observed in the mass range $115

  17. IPM measurements in the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Jansson, Andreas; Bowie, K.; Fitzpatrick, T.; Kwarciany, R.; Lundberg, C.; Slimmer, D.; Valerio, L.; Zagel, James; /Fermilab

    2007-06-01

    Two Ionization Profile Monitors (IPMs) were installed in the Tevatron in 2006. The detectors are capable of resolving single bunches turn-by-turn. This paper presents recent improvements to the system hardware and its use for beam monitoring. In particular, the correction of beam size oscillations observed at injection is discussed.

  18. Leptoquark search at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Strohmer, Raimund; /Munich U.

    2004-12-01

    This article summarizes the status of the Tevatron Run II searches for leptoquarks in p{bar p} collisions at {radical}s = 1.96 TeV. The analyses discussed use datasets with integrated luminosities ranging from 72 pb{sup -1} to 200 pb{sup -1}.

  19. Jet properties at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    D' Onofrio, Monica; /Barcelona, IFAE

    2006-07-01

    The RunII physics program at the Tevatron started in spring 2001 with protons and antiprotons colliding at an energy of {radical}s = 1.96 TeV. More than 1 fb{sup -1} of data have been collected by both the CDF and D0 experiments. In this contribution, some of the new QCD results are presented.

  20. Leptoquark searches at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Maeshima, K.

    1996-11-01

    We present recent results of searches for leptoquarks at the two Tevatron collider experiments, CDF and D{null} at Fermilab. Described here are results from direct leptoquark searches in all three generations, and indirect searches for Pati-Salam leptoquarks using rare {ital B{sub s}{sup 0}} and {ital B{sub d}{sup 0}} decay signatures.

  1. Higgs physics at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Margaroli, Fabrizio

    2014-09-15

    We show the latest results from the CDF and D0 collaborations on the study of the Higgs boson, stemming from the analysis of the entire Tevatron Run\\,II dataset. Combining the results of many individual analyses, most of which use the full data set available, an excess with a significance of approximately three standard deviations with respect to the Standard Model hypothesis is observed at a Higgs boson mass of 125\\,GeV/$c^2$. The Tevatron unique environment allows in addition to study for the first time the spin-parity hypothesis of the Higgs boson in events where it decays to quarks. Within the current experimental uncertainties, the newly discovered boson behaves as expected by the SM in the fermionic sector.

  2. Tevatron Beam Position Monitor Upgrade

    CERN Document Server

    Wolbers, Stephen; Barker, B; Bledsoe, S; Boes, T; Bowden, Mark; Cancelo, Gugstavo I; Dürling, G; Forster, B; Haynes, B; Hendricks, B; Kasza, T; Kutschke, Robert K; Mahlum, R; Martens, Michael A; Mengel, M; Olsen, M; Pavlicek, V; Pham, T; Piccoli, Luciano; Steimel, Jim; Treptow, K; Votava, Margaret; Webber, Robert C; West, B; Zhang, D

    2005-01-01

    The Tevatron Beam Position Monitor (BPM) readout electronics and software have been upgraded to improve measurement precision, functionality and reliability. The original system, designed and built in the early 1980s, became inadequate for current and future operations of the Tevatron. The upgraded system consists of 960 channels of new electronics to process analog signals from 240 BPMs, new front-end software, new online and controls software, and modified applications to take advantage of the improved measurements and support the new functionality. The new system reads signals from both ends of the existing directional stripline pickups to provide simultaneous proton and antiproton position measurements. Measurements using the new system are presented that demonstrate its improved resolution and overall performance.

  3. B States at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Paulini, Manfred; /Carnegie Mellon U.

    2009-06-01

    The CDF and D0 experiments have produced a wealth of heavy flavor physics results since the beginning of RunII of the Fermilab Tevatron. They review recent measurements of B hadron states including excited B states (B**, B{sub s}**) and the B{sub c}{sup +} meson. They also summarize the discoveries of the {Sigma}{sub b} baryon states and the {Xi}{sub b}{sup -} baryon.

  4. Diboson physics at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Neubauer, Mark S.; /UC, San Diego

    2006-05-01

    At the Fermilab Tevatron, the CDF and D0 detectors are being used to study diboson production in p{bar p} collisions at {radical}s = 1.96 TeV. The authors summarize recent measurements of the W{gamma}, Z{gamma}, and WW cross-sections and limits on WZ and ZZ production. Limits on anomalous trilinear gauge couplings are also presented.

  5. Hot topics from the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Glenzinski, D.; /Fermilab

    2008-01-01

    The Tevatron Run-II began in March 2001. To date, both the CDF and D0 experiments have collected 1 fb{sup -1} of data each. The results obtained from this data set were summarized at this conference in 39 parallel session presentations covering a wide range of topics. The author summarizes the most important of those results here and comments on some of the prospects for the future.

  6. Electroweak results from the tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Wood, D. [Fermi National Accelerator Laboratory, Batavia, IL (United States)

    1997-01-01

    Electroweak results are presented from the CDF and DO experiments based on data collected in recent runs of the Fermilab Tevatron Collider. The measurements include the mass and width of the W boson, the production cross sections of the W and Z bosons, and the W charge asymmetry. Additional results come from studies of events with pairs of electroweak gauge bosons and include limits on anomalous couplings.

  7. Top Quark Mass Measurements at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Peters, Reinhild Yvonne [DESY

    2014-01-01

    Since the discovery of the top quark in 1995 by the CDF and D0 collaborations at the Fermilab Tevatron proton antiproton collider, precise measurements of its mass are ongoing. Using data recorded by the D0 and CDF experiment, corresponding to up to the full Tevatron data sample, top quark mass measurements performed in different final states using various extraction techniques are presented in this article. The recent Tevatron top quark mass combination yields m_t=173.20 +-0.87 GeV. Furthermore, measurements of the top antitop quark mass difference from the Tevatron are discussed.

  8. Recent QCD Results from the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Vellidis, Costas [Fermilab

    2015-10-10

    Four years after the shutdown of the Tevatron proton-antiproton collider, the two Tevatron experiments, CDF and DZero, continue producing important results that test the theory of the strong interaction, Quantum Chromodynamics (QCD). The experiments exploit the advantages of the data sample acquired during the Tevatron Run II, stemming from the unique pp initial state, the clean environment at the relatively low Tevatron instantaneous luminosities, and the good understanding of the data sample after many years of calibrations and optimizations. A summary of results using the full integrated luminosity is presented, focusing on measurements of prompt photon production, weak boson production associated with jets, and non-perturbative QCD processes.

  9. Operations of the Tevatron Electron Lenses

    CERN Document Server

    Zhang, X L; Valishev, A; Stancari, G; Kuznetsov, G; Saewert, G; Kamerdzhiev, V

    2012-01-01

    The two Tevatron Electron Lenses (TEL1 and TEL2) are installed in Tevatron in 2001 and 2006 respectively. TEL1 is operated as the vital parts of the Tevatron for abort gap beam clearing, while TEL2 is functioning as the backup as well as the test device for beam-beam compensation, space charge compensator and soft beam collimator. Both of them are working exceptionally reliable after a few initial kinks being worked out. Their operations in Tevatron are summarized in this report.

  10. Jet physics at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    S. Seidel

    2002-05-29

    Recent analyses by the CDF and D0 Collaborations of jet data produced in p{bar p} collisions at the Fermilab Tevatron Collider are presented. These include new studies of the inclusive jet production cross section, a measurement of the strong coupling constant, the first measurement of subjet multiplicity of quark and gluon jets, examination of ratios of multijet cross sections and their implications for choice of renormalization scale, and a study of charged jet evolution and energy flow in the underlying event. The results are compared to theoretical predictions.

  11. Bs Mixing at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Gomez-Ceballos, Guillelmo; /Cantabria Inst. of Phys.

    2006-04-01

    The Tevatron collider at Fermilab provides a very rich environment for the study of B{sub s} mesons. B{sub s} Mixing is the most important analysis within the B Physics program of both experiments. In this paper they summarize the most recent results on this topic from both D0 and CDF experiments. There were very important updates in both experiments after his last talk, hence the organizers warmly recommended me to include the latest available results on B{sub s} mixing, instead of what he presents there.

  12. Evaluation épidémiologique du programme genevois de dépistage du cancer du sein : 2007-2011

    OpenAIRE

    2014-01-01

    A l'instar de nombreux pays industrialisés, le cancer du sein est à Genève le cancer le plus fréquent (environ 460 cas par an) et la première cause de décès chez les femmes entre 45 et 55 ans. Depuis mars 1999, le Programme genevois de dépistage du cancer du sein a pour missions de promouvoir, d'organiser et de mener une action de prévention auprès de la population féminine du canton âgée de 50 à 69 ans. Ce rapport décrit l'évolution de 15 ans d'activité de dépistage (chapitre 2) et analys...

  13. Usages et préférences de design concernant les podcasts audio professionnels : enquête auprès des professionnels des TIC

    Directory of Open Access Journals (Sweden)

    Manon Paladino-Christin

    2016-01-01

    Full Text Available Alors que l’offre de podcasts audio professionnels a explosé ces dernières années, la recherche s’est encore peu intéressée à ce nouvel objet. Sur la base du cadre d’analyse de Tsagkias, Larson, Weerkamp et de Rijke (2008, une enquête par questionnaire a été menée auprès de professionnels des technologies de l’information et de la communication pour mieux connaître les usages et les préférences de design des utilisateurs réguliers de podcasts audio. Les résultats obtenus sur un échantillon final de 53 répondants ont révélé un usage intensif du podcast (en moyenne 5 heures hebdomadaires et ont permis la mise en lumière d’éléments de préférences design fortement plébiscités par les auditeurs.

  14. Beam instrumentation for the Tevatron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Moore, Ronald S.; Jansson, Andreas; Shiltsev, Vladimir; /Fermilab

    2009-10-01

    The Tevatron in Collider Run II (2001-present) is operating with six times more bunches and many times higher beam intensities and luminosities than in Run I (1992-1995). Beam diagnostics were crucial for the machine start-up and the never-ending luminosity upgrade campaign. We present the overall picture of the Tevatron diagnostics development for Run II, outline machine needs for new instrumentation, present several notable examples that led to Tevatron performance improvements, and discuss the lessons for future colliders.

  15. Tevatron Electron Lenses: Design and Operation

    Energy Technology Data Exchange (ETDEWEB)

    Shiltsev, Vladimir; /Fermilab; Bishofberger, Kip; /Los Alamos; Kamerdzhiev, Vsevolod; /Fermilab; Kozub, Sergei; /Serpukhov, IHEP; Kufer, Matthew; Kuznetsov, Gennady; Martinez, Alexander; Olson, Marvin; Pfeffer, Howard; Saewert, Greg; Scarpine, Vic; /Fermilab /SLAC /Fermilab /Serpukhov, IHEP /Novosibirsk, IYF /Serpukhov, IHEP /Fermilab

    2008-08-01

    The beam-beam effects have been the dominating sources of beam loss and lifetime limitations in the Tevatron proton-antiproton collider [1]. Electron lenses were originally proposed for compensation of electromagnetic long-range and head-on beam-beam interactions of proton and antiproton beams [2]. Results of successful employment of two electron lenses built and installed in the Tevatron are reported in [3,4,5]. In this paper we present design features of the Tevatron electron lenses (TELs), discuss the generation of electron beams, describe different modes of operation and outline the technical parameters of various subsystems.

  16. Normal form analysis of the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Holt, J.A.

    1994-07-01

    A systematic analysis effort is under way to calculate and model the effects of present and future upgrades to the Tevatron. As a first step, using normal form theory, amplitude-dependent tuneshifts for current Tevatron collider operating conditions were calculated. The normal form algorithm was implemented within the frame work of the object-oriented accelerator physics class libraries BEAMLINE and MXYZPTLK under development at Fermilab.

  17. Top pair production distributions at the Tevatron

    Directory of Open Access Journals (Sweden)

    Takeuchi Yuji

    2013-05-01

    Full Text Available At the Tevatron, the top quark is mainly produced in pairs through the strong interaction and decays before forming hadrons. Thus the kinematical distributions at top pair production possess rich information on the tt¯$tar t$ production vertex including polarizations of top and anti-top quarks. In this article, recent measurements on top quark pair production distributions at Tevatron (CDF and DO are presented.

  18. Top physics at the Tevatron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Margaroli, Fabrizio; /Purdue U.

    2007-10-01

    The top quark has been discovered in 1995 at the CDF and DO experiments located in the Tevatron ring at the Fermilab laboratory. After more than a decade the Tevatron collider, with its center-of-mass energy collisions of 1.96 TeV, is still the only machine capable of producing such exceptionally heavy particle. Here I present a selection of the most recent CDF and DO measurements performed analyzing {approx} 1 fb{sup -1} of integrated luminosity.

  19. L’Association du personnel, le TREF, le Comité des Finances et le Conseil du CERN

    CERN Multimedia

    Staff Association

    2016-01-01

    L’Association du personnel, forte de son approche participative et consensuelle, recherche toujours le meilleur accord possible pour l’Organisation et son personnel. Pour ce faire, discussions et concertation avec la Direction, travail d’explication et de persuasion au TREF et ailleurs auprès des délégués des États membres sont nos principaux atouts. TREF (Tripartite Employment Conditions Forum), un Forum d’échanges, de discussions « L’objectif du Forum est d’améliorer le processus de prise de décision  en donnant aux personnes concernées la possibilité et le temps de comprendre pleinement la position de tous les participants. » (CERN/RTG/8) Le Forum tripartite sur les conditions d’emploi (TREF), créé par le Conseil du CERN en juin 1994, est composé de r...

  20. From the Tevatron to Project X

    CERN Multimedia

    Pier Oddone, Fermilab director (from CERN Courier)

    2011-01-01

    In the October issue of the CERN Courier, Fermilab Director Pier Oddone will present the past, present and future of the US laboratory after the Tevatron. The Bulletin presents some early extracts from his article…   Fermilab Director, Pier Oddone. The end of September marks the end of an era at Fermilab, with the shutdown of the Tevatron after 28 years of operation at the frontiers of particle physics. The Tevatron’s far-reaching legacy spans particle physics, accelerator science and industry. The collider established Fermilab as a world leader in particle physics research, a role that will be strengthened with a new set of facilities, programmes and projects in neutrino and rare-process physics, astroparticle physics, and accelerator and detector technologies. The Tevatron exceeded every expectation ever set for it. This remarkable machine achieved luminosities with antiprotons once considered impossible, reaching more than 4x1032 cm-2s-1 instantaneous luminosity and...

  1. Elastic scattering tracking at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Avila, C. [Cornell Univ., Ithaca, NY (United States); Baker, W. [Fermi National Accelerator Laboratory, Batavia, IL (United States); DeSalvo, R. [European Organization for Nuclear Research, Geneva (Switzerland); Eartly, D. [Fermi National Accelerator Laboratory, Batavia, IL (United States); Guss, C. [Cornell Univ., Ithaca, NY (United States); Jostlein, H. [Fermi National Accelerator Laboratory, Batavia, IL (United States); Lundin, M. [Universite Louis Pasteur and CRN, Strasbourg (France); Mondardini, M.R. [Cornell Univ., Ithaca, NY (United States); Orear, J. [Cornell Univ., Ithaca, NY (United States)

    1995-06-01

    Tracks have been observed for the first time with a new scintillating fibers and image intensifiers based detector mounted directly inside the vacuum of the Tevatron collider to study pp{sup -} small angle scattering at {radical}(s)=1.8 TeV. This detector was conceived and developed at CERN and built at DEP for elastic scattering measurements at the Tevatron and future colliders. Two pairs of such detectors, symmetric in the vertical plane, will be located along the beam pipe at either side from the interaction point E0 in the Tevatron. The first detector has been recently installed by the E811 collaboration and is being tested with beam halo. Another one is being tested in a cosmic ray setup. Preliminary results are presented from both configurations and agree with preliminary tests performed at CERN/PS. (orig.).

  2. Top quark mass measurement at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Guimaraes da Costa, Joao; /Harvard U.

    2004-12-01

    The authors report on the latest experimental measurements of the top quark mass by the CDF and D0 Collaborations at the Fermilab Tevatron. They present a new top mass measurement using the t{bar t} events collected by the D0 Collaboration in Run I between 1994 and 1996. This result is combined with previous measurements to yield a new world top mass average. They also describe several preliminary results using up to 193 pb{sup -1} of t{bar t} events produced in {bar p}p collisions at {radical}s = 1.96 TeV during the Run II of the Tevatron.

  3. The Hunt for Supersymmetry at the Tevatron

    Directory of Open Access Journals (Sweden)

    André Sopczak

    2014-03-01

    Full Text Available During the Tevatron data-taking period from April 2001 to September 2011 (Run-II, several searches for supersymmetric particles were performed. The results from searches by the CDF and DØ collaborations are concisely reviewed. This includes results up to the summer conferences of 2013. Model-independent and model-dependent limits on new particle production are set, and interpretations in supersymmetric models are given. Several limits from the Large Electron Positron (LEP era have been extended. Specific results are placed into the context of the Tevatron performance expectations and a few of the current results from searches at the Large Hadron Collider (LHC.

  4. Channeling collimation studies at the Fermilab Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Carrigan, Richard A.; Drozhdin, Alexandr I.; Fliller, Raymond P., III; Mokhov, Nikolai V.; Shiltsev, Vladimir D.; Still, Dean A.; /Fermilab

    2006-08-01

    Bent crystal channeling has promising advantages for accelerator beam collimation at high energy hadron facilities such as the LHC. This significance has been amplified by several surprising developments including multi-pass channeling and the observation of enhanced deflections over the entire arc of a bent crystal. The second effect has been observed both at RHIC and recently at the Tevatron. Results are reported showing channeling collimation of the circulating proton beam halo at the Tevatron. Parenthetically, this study is the highest energy proton channeling experiment ever carried out. The study is continuing.

  5. Top and Electroweak Measurements at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Bartos, P. [Comenius U.

    2016-01-01

    In this report, we summarize the latest results of the top-quark mass and electroweak measurements from the Tevatron. Since the world combination of top-quark mass measurements was done, CDF and D0 experiments improved the precision of several results. Some of them reach the relative precition below 1% for a single measurement. From the electroweak results, we report on the WW and WZ production cross section, measurements of the weak mixing angle and indirect measurements of W boson mass. The Tevatron results of the weak mixing angle are still the most precise ones of hadron colliders.

  6. Single Z Production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Phillips, Thomas J.

    2012-05-01

    The production of single Z bosons has been studied at Fermilab's Tevatron by the CDF and D0 collaborations. Measurements include the weak mixing angle, vector and axial-vector couplings between Z bosons and light quarks, and angular coefficients in electronic decays which are sensitive to the spin of the gluon. The collaborations have looked for and indication of new physics above the mass scale that can be directly produced at the Tevatron by studying the interference between Z and photon propagators. All measurements are consistent with Standard Model expectations.

  7. B(s) properties at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Gomez-Ceballos, Guillelmo; /Cantabria U., Santander

    2005-11-01

    The Tevatron collider at Fermilab provides a very rich environment for the study B{sub s} mesons. In this paper they show a few selected topics from the CDF and D0 collaborations, giving special attention to the B{sub s} Mixing analyses. This note corresponds to the proceedings of the Hadron Collider Physics 2005 conference.

  8. Tevatron targets three-year extension

    CERN Document Server

    Harris, Margaret

    2010-01-01

    "Fermilab's Tevatron collider could get a new lease on life following a campaign to keep the facility running beyond the end of 2011, when the rival Large Hadron Collider (LHC) at Cern is scheduled to shut down for 15 months of repairs" (0.75 page)

  9. WW and WZ production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Lipeles, Elliot; /UC, San Diego

    2007-01-01

    This report summarizes recent measurements of the production properties of WW and WZ pairs of bosons at the Tevatron. This includes measurements of the cross-section and triple gauge couplings in the WW process and the first evidence for WZ production.

  10. Photon final states at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Campanelli, Mario; /University Coll. London

    2008-04-01

    The authors present here several recent measurements involving associate production of photons and jets at the Tevatron. In particular, inclusive photon + met from D0, and photon + b-jets and photon + b-jet + leptons + MET from CDF are described in some detail. These measurements offer a good test of QCD predictions in rather complex final states.

  11. Fermilab Tevatron and Pbar source status report

    Energy Technology Data Exchange (ETDEWEB)

    Edwards, H.

    1986-08-01

    The antiproton production cycle is enumerated, and the commissioning of the antiproton source is described, giving milestones and major obstacles. The Tevatron collider operation is described, including procedure to load the Tevatron with three bunches of protons and three bunches of antiprotons. Commissioning of the Main Ring and Tevatron for collider operation is described. Development and accelerator studies in four areas were necessary: main ring RF manipulations; controls and applications software support; Tevatron storage and low-beta squeeze sequence; and study of various beam transfers, storage steps, and sequences. Final tests are described. A long range upgrade program is presently under evaluation to accomplish these goals: luminosity increase to 5 x 10/sup 31/ cm/sup -2/sec/sup -1/, production rates up to 4 x 10/sup 11/ antiprotons/hr, and intensity increase for fixed target operation. Beam quality is to be improved by the injector and main ring upgrades, and the luminosity goal is addressed by the Collider upgrade. (LEW)

  12. Jet fragmentation properties at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Goulianos, K. [The Rockefeller University, NY, NY (United States); CDF Collaboration

    1997-05-16

    Preliminary CDF results on inclusive momentum distributions of charged particles in high transverse momentum jets produced in {anti p}p collisions at {radical}s=1.8 TeV at the Tevatron are presented and compared with QCD predictions based on the Modified Leading Log Approximation.

  13. Tevatron sees light at end of tunnel?

    CERN Multimedia

    Seife, C

    2002-01-01

    Physicists at Fermilab are finally starting to get on top of problems with the beam luminosity of the Tevatron. After a million dollar refit last year, every single luminosity target has been missed since it went operational six months ago (1 page).

  14. Theoretical Issues in the Tevatron Era

    CERN Document Server

    Rosner, Jonathan L

    2000-01-01

    The Fermilab Tevatron's operation for fixed-target physics from its start in 1983 until the end of fixed-target running in 2000 was marked by extraordinary peoductivity and variety. Some of the changing theoretal issues associated with this program are reviewed.

  15. Tevatron Electron Lenses: Design and Operation

    Energy Technology Data Exchange (ETDEWEB)

    Shiltsev, Vladimir; /Fermilab; Bishofberger, Kip; /Los Alamos; Kamerdzhiev, Vsevolod; /Fermilab; Kozub, Sergei; /Serpukhov, IHEP; Kufer, Matthew; Kuznetsov, Gennady; Martinez, Alexander; Olson, Marvin; Pfeffer, Howard; Saewert, Greg; Scarpine, Vic; /Fermilab; Seryi, Andrei; /SLAC; Solyak, Nikolai; /Fermilab; Sytnik, Veniamin; /Serpukhov, IHEP; Tiunov, Mikhail; /Novosibirsk, IYF; Tkachenko, Leonid; /Serpukhov, IHEP; Wildman, David; Wolff, Daniel; Zhang, Xiao-Long; /Fermilab

    2011-09-12

    Fermilab's Tevatron is currently the world's highest energy accelerator in which tightly focused beams of 980 GeV protons and antiprotons collide at two dedicated interaction points (IPs). Both beams share the same beam pipe and magnet aperture and, in order to avoid multiple detrimental head-on collisions, the beams are placed on separated orbits everywhere except the main IPs by using high-voltage (HV) electrostatic separators. The electromagnetic beam-beam interaction at the main IPs together with the long-range interactions between separated beams adversely affect the collider performance, reducing the luminosity integral per store (period of continuous collisions) by 10-30%. Tuning the collider operation for optimal performance becomes more and more cumbersome as the beam intensities and luminosity increase. The long-range effects which (besides being nonlinear) vary from bunch to bunch are particularly hard to mitigate. A comprehensive review of the beam-beam effects in the Tevatron Collider Run II can be found in Ref. [1]. The beam-beam effects have been the dominating sources of beam loss and lifetime limitations in the Tevatron proton-antiproton collider [1]. Electron lenses were originally proposed for compensation of electromagnetic long-range and head-on beam-beam interactions of proton and antiproton beams [2]. Results of successful employment of two electron lenses built and installed in the Tevatron are reported in [3,4,5]. In this paper we present design features of the Tevatron electron lenses (TELs), discuss the generation of electron beams, describe different modes of operation and outline the technical parameters of various subsystems.

  16. Mesure de la production de di-bosons WZ auprès du LHC avec l'experience ATLAS

    CERN Document Server

    Keoshkerian, Houry

    This thesis is performed in the frame of the ATLAS experiment at the LHC. A first part of the work presented in this document consists on the time calibration of the ATLAS Liquid Argon (LAr) calorimeter. The control of the time alignment of the calorimeter is important for the goodness of the quality of the energy reconstructed in the calorimeter. The results presented in this thesis have allowed an improvement of 30% of the global time resolution of the LAr calorimeter. The Standard model of particle physics predicts, during proton collisions, the production of the $W$ and $Z$ weak bosons as a pair due to the interaction of a quark with an anti-quark. The diboson production can be sensitive to the couplings between vector bosons. An anomalous deviation of these couplings from the prediction of the SM would point to the presence of new physics. The use of the full statistics of the 2012 ATLAS data allowed us to increase the precision of the measurement of these couplings compared to previous results based on...

  17. Recherche de particules supersymetriques dans le canal jets et energie transverse manquante aupres du detecteur ATLAS au LHC

    CERN Document Server

    Niedercorn, Francois

    The main topic of this thesis is the search for supersymmetric particles in the specific frame of the mSUGRA model at the LHC with the ATLAS detector. The search is based on data taken between 2010 and 2011. This document presents also some of the works made upstream by the ATLAS collaboration in order to obtain these results.

  18. Achieving high luminosity in the Fermilab Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Holmes, S.D.

    1991-05-01

    Fermilab has embarked upon a program, christened Fermilab III, to raise the luminosity in the Tevatron proton-antiproton collider over the next five years by at least a factor of thirty beyond the currently achieved level of 1.6{times}10{sup 30}cm{sup {minus}2}sec{sup {minus}1}. Components of the program include implementation of electrostatic separators, Antiproton Source improvements, installation of cold compressors, doubling the existing linac output energy, and the construction of a new accelerator--the Fermilab Main Injector. Basic limitations in the achievement of higher luminosity in the Tevatron, the strategy developed to achieve the Fermilab III goals, and the evolution of luminosity throughout the period will be discussed. 1 fig., 2 tabs.

  19. Tevatron accelerator physics and operation highlights

    CERN Document Server

    Valishev, A

    2011-01-01

    The performance of the Tevatron collider demonstrated continuous growth over the course of Run II, with the peak luminosity reaching 4\\times1032 cm-2 s-1, and the weekly integration rate exceeding 70 pb-1. This report presents a review of the most important advances that contributed to this performance improvement, including beam dynamics modeling, precision optics measurements and stability control, implementation of collimation during low-beta squeeze. Algorithms employed for optimization of the luminosity integration are presented and the lessons learned from high-luminosity operation are discussed. Studies of novel accelerator physics concepts at the Tevatron are described, such as the collimation techniques using crystal collimator and hollow electron beam, and compensation of beam-beam effects.

  20. Novel tune diagnostics for the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Tan, Cheng-Yang; /Fermilab

    2005-04-01

    In the Tevatron collider, protons and antiprotons share the same beam pipe. This poses a challenge in the measurement of tunes for both species simultaneously because of the possibility of signal contamination from the other species. The tune of each bunch is also very different because of beam-beam effects from parasitic crossing points. This means that the tune diagnostics must be able to differentiate between protons and anti-protons, it also has to measure tunes from each bunch. There are three different tune pickups used in the Tevatron: 1.7 GHz Schottky pickups, 21.4 MHz Schottky pickups and baseband pickups. These devices will be discussed in detail in this paper.

  1. Higgs results from the Tevatron Run II

    Energy Technology Data Exchange (ETDEWEB)

    Tuchming, B.; /DAPNIA, Saclay

    2005-01-01

    The data taken at the Tevatron experiments have been analyzed to search for Higgs bosons. For the Standard Model Higgs searches, no excess is observed, the data are in good agreement with the expectations, so that limits are set on the production rates. For various theoretical models beyond the Standard Model, there is no excess either, which allows to derive constraints in their respective parameter spaces.

  2. Recent QCD Studies at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Group, Robert Craig

    2008-04-01

    Since the beginning of Run II at the Fermilab Tevatron the QCD physics groups of the CDF and D0 experiments have worked to reach unprecedented levels of precision for many QCD observables. Thanks to the large dataset--over 3 fb{sup -1} of integrated luminosity recorded by each experiment--important new measurements have recently been made public and will be summarized in this paper.

  3. Heavy Flavor Baryons at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Kuhr, Thomas

    2011-09-01

    The Tevatron experiments CDF and D0 have filled many empty spots in the spectrum of heavy baryons over the last few years. The most recent results are described in this article: The first direct observation of the {Xi}{sub b}{sup 0}, improved measurements of {Sigma}{sub b} properties, a new measurement of the {Lambda}{sub b} {yields} J/{psi}{Lambda} branching ratio, and a high-statistics study of charm baryons.

  4. $B$ mixing and lifetimes at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Gomez-Ceballos, G.; Piedra, J.

    2006-04-01

    The Tevatron collider at Fermilab provides a very rich environment for the study of b-hadrons. Both the D0 and CDF experiments have collected a sample of about 1 fb{sup -1}. they report results on three topics: b-hadron lifetimes, polarization amplitudes and the decay width difference in B{sub s}{sup 0} {yields} J/{psi}{phi}, and B{sub s}{sup 0} mixing.

  5. Searching for Gluinos at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Alwall, Johan; Le, My-Phuong; Lisanti, Mariangela; Wacker, Jay G.; /SLAC /Stanford U., Phys. Dept.

    2008-03-14

    This letter describes how to perform model-independent searches for new pair-produced color octet particles that each subsequently decay into two jets plus missing energy at the Tevatron. Current searches are not sensitive to all regions of parameter space because they employ CMSSM-motivated cuts. Optimizing the H{sub T} and E{sub T} cuts expands the sensitivity of searches for all kinematically allowed decays.

  6. Review of Tevatron Results: Top quark physics

    CERN Document Server

    Gerber, Cecilia E

    2014-01-01

    We present results on top quark physics from the CDF and D0 collaborations at the Fermilab Tevatron proton anti-proton collider. These include legacy results from Run II that were published or submitted for publication before mid-2014, as well as a summary of Run I results. The historical perspective of the discovery of the top quark in Run I is also described.

  7. Di-boson production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    De Lentdecker, Gilles; /Rochester U.

    2005-05-01

    The authors present some precision measurements on electroweak physics performed at the Tevatron collider at Fermilab. Namely they report on the boson-pair production cross sections and on triple gauge boson couplings using proton anti-proton collisions collected by the CDF and D0 experiments at the center-of-mass energy of 1.96 TeV. The data correspond to an integrated luminosity of up to 324 pb{sup -1}.

  8. Top Quark Pair Production Cross Section at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Peters, Reinhild Yvonne [Manchester U.

    2015-09-25

    The top quark, discovered in 1995 by the CDF and D0 collaborations at the Tevatron proton antiproton collider at Fermilab, has undergone intense studies in the last 20 years. Currently, CDF and D0 converge on their measurements of top-antitop quark production cross sections using the full Tevatron data sample. In these proceedings, the latest results on inclusive and differential measurements of top-antitop quark production cross sections at the Tevatron are reported.

  9. Longitudinal dynamics and tomography in the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Stogin, J. [Princeton Univ., Princeton, NJ (United States); Sen, T. [Fermi National Accelerator Laboratory (FNAL), Batavia, IL (United States); Moore, R. S. [Fermi National Accelerator Laboratory (FNAL), Batavia, IL (United States)

    2012-01-10

    Motivated by the desire to understand the longitudinal effects of beam-beam forces, we study the longitudinal dynamics of protons and anti-protons at injection and top energy in the Tevatron. Multi-turn data of the longitudinal profiles are captured to reveal information about frequencies of oscillation, and changes in the bunch distributions. Tomographic reconstruction is used to create phase space maps which are subsequently used to find the momentum distributions. Changes in these distributions for both proton and anti-proton beams are also followed through the operational cycle. We report too on the details of interesting dynamics and some unexpected findings.

  10. Non SUSY Searches at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Cortabitarte, R. Vilar

    2004-08-26

    The Fermilab Tevatron collider experiments, CDF and D0, have collected {approx} 200 pb{sup -1} of data at {radical}s = 1.96 TeV since March 2002 (RunII). Both experiments have investigated physics beyond the standard model; this paper reviews some of the recent results on the searches for new phenomena, concentrating on Z', extra dimensions, excited electrons and lepto quarks. No signal was observed, therefore stringent limits on the signatures and models were derived.

  11. B lifetimes and mixing at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Bedeschi, Franco; /INFN, Pisa

    2005-05-01

    The authors present recent results on b-hadron lifetimes and mixing obtained from the analysis of the data collected at the Tevatron Collider by the CDF and D0 Collaborations in the period 2002-2004. Many lifetime measurements have been updated since the Summer 2004 conferences, sometimes improving significantly the accuracy. Likewise the measurement of the B{sub d} oscillation frequency has been updated. New limits on the B{sub s} oscillation frequency have been determined using for the first time Run II data.

  12. Recent Tevatron Results on CP-Violation

    Energy Technology Data Exchange (ETDEWEB)

    Garbincius, Peter H. [Fermilab

    2014-08-27

    Using their full Tevatron Run II data sets, the CDF and D0 Experiments present measurements of CP -violating asymmetries in the charmless decays of bottom baryons Λ0 → pπ-, Λ0 → pK-, and also for B0 → K-π+, B0 → K+π-, b b s Ds → φπ± , and for single muons and like-sign dimuons in pp collisions. Except for the like-sign dimuon asymmetry, these asymmetry measurements are consistent with available predictions of the standard model.

  13. Recent Tevatron Results on CP-Violation

    Energy Technology Data Exchange (ETDEWEB)

    Garbincius, Peter H. [Fermilab

    2014-08-25

    Using their full Tevatron Run II data sets, the CDF and D0 Experiments present measurements of CP-violating asymmetries in the charmless decay of bottom baryons Lambda-b => p pi-, Lambda-b => p K-, and also for Bs0 => K- pi+, B0 => K+ pi-, Ds => phi pi, and for single muons and like-sign dimuons in p-pbar collisions. Except for the like-sign dimuon asymmetry, these asymmetry measurements are consistent with available predictions of the standard model.

  14. Search for MSSM Higgses at the Tevatron

    CERN Document Server

    Connolly, A

    2002-01-01

    We present an overview of searches for MSSM Higgs at the Tevatron, concentrating on searches probing the high tan(beta) region. We discuss the search for A/H -> tau tau which is soon to be completed in the Run I data and review the new tau triggers implemented by CDF and D0 in Run II, which will greatly impact this analysis. We also present the results of a Run I search for A/H bb -> bbbb performed by CDF and highlight expected improvements in this channel by both experiments in Run II.

  15. New diffractive results from the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Gallinaro, Michele; /Rockefeller U.

    2005-05-01

    Experimental results in diffractive processes are summarized and a few notable characteristics described in terms of Quantum Chromodynamics. Exclusive dijet production is used to establish a benchmark for future experiments in the quest for diffractive Higgs production at the Large Hadron Collider. Using new data from the Tevatron and dedicated diffractive triggers, no excess over a smooth falling distribution for exclusive dijet events could be found. Stringent upper limits on the exclusive dijet production cross section are presented. The quark/gluon composition of dijet final states is used to provide additional hints on exclusive dijet production.

  16. Prompt photon production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Kumar, Ashish; /SUNY, Stony Brook

    2009-07-01

    Prompt photon production has been studied by the CDF and D0{sup -} experiments at the Fermilab Tevatron collider in p{bar p} collisions at the centre of mass energy of {radical}s = 1.96 TeV. Measurements of the inclusive photon, inclusive photon plus jet, photon plus heavy flavor jet, and diphoton production cross sections are discussed. The analyses use data sample corresponding to integrated luminosity between 0.2 fb{sup -1} and 1.02 fb{sup -1}. The results are compared to the next to leading order (NLO) perturbative QCD (pQCD) calculations.

  17. Review of Physics Results from the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Bandurin, D. [Virginia U.; Bernardi, G. [Paris U., VI-VII; Gerber, C. [Chicago U., EFI; Junk, T. [Fermilab; Juste, A. [Barcelona, IFAE; Kotwal, A. [Duke U.; Lewis, J. [Fermilab; Mesropian, C. [Rockefeller U.; Schellman, H. [Northwestern U.; Sekaric, J. [Kansas U.; Toback, D. [Texas A-M; Van Kooten, R. [Indiana U.; Vellidis, C. [Fermilab; Zivkovic, L. [Clemson U.

    2015-02-27

    We present a comprehensive review of the physics results obtained by the CDF and D0 collaborations up to summer 2014, with emphasis on those achieved in the Run II of the Tevatron collider which delivered a total integrated luminosity of ~10 fb$^{-1}$ at $\\sqrt{s} = 1.96~{\\rm TeV}$. The results are presented in six main physics topics: QCD, Heavy Flavor, Electroweak, Top quark, Higgs boson and searches for New Particles and Interactions. The characteristics of the accelerator, detectors, and the techniques used to achieve these results are also briefly summarized.

  18. Charm (and Beauty) Production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Rademacker, Jonas; /Bristol U.

    2007-11-01

    The authors present recent results on heavy flavor production at Tevatron Run II for typically {approx} 1 fb{sup -1} of analyzed p{bar p} data at {radical}s = 1.96 TeV. This includes results on single and correlated open charm and bottom cross sections, charm pair production kinematics, J/{psi}, {psi}(2S) and {chi}{sub cJ} cross sections and polarization measurements in J/{psi}, {psi}(2S), {Upsilon}(1S), and {Upsilon}(2S).

  19. Spectroscopy and Decay of B Hadrons at the Tevatron

    CERN Document Server

    Paulini, M

    2007-01-01

    This paper reviews the spectroscopy and decay of B hadrons at the Tevatron. We discuss the spectroscopy of excited B states (B**, Bs**) and the observation of the Sigma_b baryon at the Tevatron. The second part of this review discusses the decays of B hadrons and measurements of branching fractions. We focus on charmless two-body decays of B->hh.

  20. Tevatron Results on Heavy Flavor Production and Decay

    Energy Technology Data Exchange (ETDEWEB)

    Scuri, Fabrizio [INFN, Pisa

    2014-09-02

    The most recent results on heavy flavor production and decays from the Tevatron experiments CDF and D0 are summarized and compared with some LHC experiment results. The collected data sample refers to the full Tevatron Run II operation and it corresponds to about 10 inverse fb of integrated luminosity per experiment.

  1. Elizabeth Cady Stanton. Naissance du féminisme américain à Seneca Falls

    OpenAIRE

    2016-01-01

    Cet ouvrage met en scène une double naissance : celle du féminisme américain avec le moment inaugural de la Convention de Seneca Falls en 1848, et l'émergence d’Elizabeth Cady Stanton comme force vive et tête pensante des tout premiers combats pour l’affirmation et la conquête des droits de la femme aux États-Unis. À travers des textes jamais traduits en français, on perçoit l’éveil d’une conscience, du cadre privé de l’enfance jusqu’à l’intervention publique auprès du Congrès de New York en...

  2. An Ionization Profile Monitor for the Tevatron

    CERN Document Server

    Jansson, Andreas; Bowie, Kwame; Bross, Alan; Dysert, Robert; Fitzpatrick, Thomas; Kwarciany, Richard; Lundberg, Carl; Nguyen, Hogan; Rivetta, Claudio H; Slimmer, David; Valerio, Linda; Zagel, James

    2005-01-01

    Primarily to study emittance blowup during injection and ramping, an ionization profile monitor has been developed for the Tevatron. It is based on a prototype installed in the Main Injector, although with extensive modifications. In particular, the electromagnetic shielding has been improved, the signal path has been cleaned up, and provisions have been made for an internal electron source. Due to the good Tevatron vacuum, a local pressure bump is introduced to increase the primary signal, which is then amplified by a microchannel plate and detected on anode strips. For the DAQ, a custom ASIC developed for the CMS experiment is used. It is a combined charge integrator and digitizer, with a sensitivity of a few fC, and a time-resolution that allows single bunch measurement. Digitization is done in the tunnel to reduce noise. Preparations for detector installation were made during the long 2004 shutdown, with the installation of magnets, vacuum chambers, vacuum pumps and cabling. The actual detector will be in...

  3. QCD, Tevatron results and LHC prospects

    Energy Technology Data Exchange (ETDEWEB)

    Elvira, V.Daniel; /Fermilab

    2008-08-01

    We present a summary of the most recent measurements relevant to Quantum Chromodynamics (QCD) delivered by the D0 and CDF Tevatron experiments by May 2008. CDF and D0 are moving toward precision measurements of QCD based on data samples in excess of 1 fb-1. The inclusive jet cross sections have been extended to forward rapidity regions and measured with unprecedented precision following improvements in the jet energy calibration. Results on dijet mass distributions, bbbar dijet production using tracker based triggers, underlying event in dijet and Drell-Yan samples, inclusive photon and diphoton cross sections complete the list of measurements included in this paper. Good agreement with pQCD within errors is observed for jet production measurements. An improved and consistent theoretical description is needed for photon+jets processes. Collisions at the LHC are scheduled for early fall 2008, opening an era of discoveries at the new energy frontier, 5-7 times higher than that of the Tevatron.

  4. Combined SM Higgs Limits at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Krumnack, N.

    2009-10-01

    We combine results from CDF and D{sup 0} on direct searches for a standard model (SM) Higgs boson (H) in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV. Compared to the previous Higgs Tevatron combination, more data and new channels WH {yields} {tau}{nu}b{bar b}, VH {yields} {tau}{tau}b{bar b}/jj{tau}{tau}, VH {yields} jjb{bar b}, t{bar t}H {yields} t{bar t}b{bar b} have been added. Most previously used channels have been reanalyzed to gain sensitivity. We use the latest parton distribution functions and gg {yields} H theoretical cross sections when comparing our limits to the SM predictions. With 2.0-3.6 fb{sup -1} of data analyzed at CDF, and 0.9-4.2 fb{sup -1} at D{sup 0}, the 95% C.L. upper limits on Higgs boson production are a factor of 2.5 (0.86) times the SM cross section for a Higgs boson mass of m{sub H} = 115 (165) GeV/c{sup 2}. Based on simulation, the corresponding median expected upper limits are 2.4 (1.1). The mass range excluded at 95% C.L. for a SM Higgs has been extended to 160 < m{sub H} < 170 GeV/c{sup 2}.

  5. Bucket shaking stops bunch dancing in Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Burov, A.; Tan, C.Y.; /Fermilab

    2011-03-01

    Bunches in Tevatron are known to be longitudinally unstable: their collective oscillations, also called dancing bunches, persist without any signs of decay. Typically, a damper is used to stop these oscillations, but recently, it was theoretically predicted that the oscillations can be stabilized by means of small bucket shaking. Dedicated measurements in Tevatron have shown that this method does stop the dancing. According to predictions of Refs. [2,3], the flattening of the bunch distribution at low amplitudes should make the bunch more stable against LLD. An experiment has been devised to flatten the distribution by modulating the RF phase at the low-amplitude synchrotron frequency for a few degrees of amplitude. These beam studies show that stabilisation really happens. After several consecutive shakings, the dancing disappears and the resulting bunch profile becomes smoother at the top. Although not shown in this report, sometimes a little divot forms at the centre of the distribution. These experiments confirm that resonant RF shaking flattens the bunch distribution at low amplitudes, and the dancing stops.

  6. Search for supersymmetric particles decaying into tri-leptons through R-parity violation, with D0 Run-II experiment at Fermilab; Recherche de particules supersymetriques se desintegrant en R-parite violee (couplage {lambda}(121)) dans un etat final a trois leptons, avec les donnees du Run-II de l'experience D0 au TeVatron

    Energy Technology Data Exchange (ETDEWEB)

    Magnan, A.M

    2005-07-15

    This thesis is dedicated to the study of the first data taken by the D0 detector during the Run II of the Tevatron. Supersymmetric particles have been search for in proton-antiproton collisions, with a center of mass energy of 1.96 TeV. In the framework of supersymmetry with R-parity violation, I have studied the pair production of Gauginos, leading to a pair of LSP (0,{chi}{sub 1}), each one decaying into ee{nu}{sub {mu}} or e{mu}{nu}{sub e} with a {lambda}(121) coupling. The final state contains at least two electrons: I have thus paid special attention in this work to the methods concerning identification and mis-identification of electromagnetic particles, as well as reconstruction, triggering, and correction (of the reconstructed energy). In a selection of tri-leptons, with at least two electrons, and some transverse missing energy, we observed 0 event in the 350 pb{sup -1} of analyzed data, for 0.4 + 0.35 - 0.05 (sta) {+-} 0.16 (sys) expected from the Standard Model contributions. In the signal considered in this analysis, the selection efficiency is around 12 per cent. Results have been studied in two models: mSUGRA and MSSM. In mSUGRA model, limits on m(1/2) and lightest gauginos's masses have been obtained, with tan({beta}) = 5, A{sub 0} = 0, m{sub 0} = 100 and 1000 GeV.c{sup -2} and both signs of {mu}. In MSSM, with the hypothesis of massive sfermions (1000 GeV.c{sup -2}), we can exclude, at 95% Confidence Level, the region m({chi}{sub 1}{sup {+-}}) < 200 GeV.c{sup -2} for all masses of {chi}{sub 1}{sup 0} LSP. (author)

  7. Professionnalisation et développement professionnel des enseignants dans un contexte d’intégration des TICE : le cas du Québec

    OpenAIRE

    Karsenti, Thierry; Grégoire, Pascal

    2015-01-01

    Contexte La question de la professionnalisation et du développement professionnel des formateurs universitaires du Québec dans un contexte d’intégration des TICE revêt plusieurs défis. En effet, même si les formateurs universitaires forment des enseignants du primaire et du secondaire aux TICE, de même qu’aux usages pédagogiques des TICE auprès des élèves, ils ne sont, eux, pas tenus d’être formés dans ce domaine. Autrement dit, dans les neuf universités du Québec qui forment de futurs maître...

  8. Performance du spectrometre a muons d’ALICE. Production et mesure des bosons faibles dans des collisions d’ions lourds aupres du LHC

    CERN Document Server

    Conesa Del Valle, Zaida; Moreno, F Fernandez

    2007-01-01

    Nucleus-nucleus collisions are the unique tool available to investigate the QCD matter phase diagram in the laboratory. A lot of work has been devoted to explore it in different domains in the last 3 decades, and the forthcoming LHC collider will contribute to such research increasing the collision center-of-mass energy by a factor 30 and the energy densities by a factor 1-10 with respect to the RHIC collider [C+04, A+06].Only a comprehensive analysis of a wide spectrum of experimental observables can help to fully characterize the prospected matter. In particular, valuable information is expected from charm and beauty production, the situation from SPS and RHIC charmonia data being puzzling [GdC07, Lei07, A+00a, Sco07], and the c¯c (b¯b) yields per central nucleon-nucleon collision being increased from 10 (0.1) to 110 (5) from RHIC to LHC [C+04, MG07]. Whether quarkonia will thermalize, will develop collective motion, will be further suppressed or regenerated are still open questions that LHC data might re...

  9. De l'expérience ALEPH au LEP à la construction du détecteur ATLAS auprès du LHC

    CERN Document Server

    Martin, Franck

    This document summarizes ten years of activities in the field of experimental particle physics, which I have done just after my PhD defense in 1999. After a short introduction describing my PhD work and my activities during these ten years, the first chapter describes an analysis made in the ALEPH experiment about the measurement of the Bose-Einstein correlations in W pair decays, using an event mixing method. Nevertheless, the main part of the text is dedicated to the work I have done in the ATLAS experiment at the LHC, between the years 2000 and 2010. Four parts are distinguished. First, an analysis concerning some searches for possible supersymmetric top decays with R-parity violation is described. Then a second part is written about the test bench of the tile calorimeter front-end electronics, and its installation in the ATLAS experiment. Third, the work done in the transition radiation tracker concerning the validation and the installation of the endcap front-end electronics is fully explained. End, the ...

  10. Groupement des anciens du CERN et de l'ESO

    CERN Multimedia

    GAC-EPA

    2011-01-01

    Le GAC organise chaque mois des permanences avec entretiens individuels. La prochaine permanence se tiendra le Mardi 8 mars de 13h30 à 16h00 Salle de conférence de l’Association du personnel Les permanences suivantes auront lieu les mardis 13 avril, 4 mai, 1er juin, 7 septembre, 5 octobre, 2 novembre et 7 décembre. Les permanences du Groupement des Anciens sont ouvertes aux bénéficiaires de la Caisse de pensions (y compris les conjoints survivants !) et à tous ceux qui approchent de la retraite. Nous invitons vivement ces derniers à s’associer à notre groupement en se procurant, auprès de l’Association du personnel, les documents nécessaires. * * * * * Le Comité du GAC-EPA vous informe de la tenue de son Assemblée générale ordinaire 2011 Vendredi 25 mars 2011 à 14h00 dans l’Amphithé&...

  11. Groupement des anciens du CERN et de l'ESO

    CERN Document Server

    GAC-EPA

    2011-01-01

    Le GAC organise chaque mois des permanences avec entretiens individuels. La prochaine permanence se tiendra le Mardi 13 avril de 13h30 à 16h00 Salle de conférence de l’Association du personnel Les permanences suivantes auront lieu les mardis 4 mai, 1er juin, 7 septembre, 5 octobre, 2 novembre et 7 décembre. Les permanences du Groupement des Anciens sont ouvertes aux bénéficiaires de la Caisse de pensions (y compris les conjoints survivants !) et à tous ceux qui approchent de la retraite. Nous invitons vivement ces derniers à s’associer à notre groupement en se procurant, auprès de l’Association du personnel, les documents nécessaires. * * * * * Le Comité du GAC-EPA vous informe de la tenue de son Assemblée générale ordinaire 2011 Vendredi 25 mars 2011 à 14h00 dans l’Amphith&e...

  12. Diagnostics of the Fermilab Tevatron using an AC dipole

    Energy Technology Data Exchange (ETDEWEB)

    Miyamoto, Ryoichi [Univ. of Texas, Austin, TX (United States)

    2008-08-01

    The Fermilab Tevatron is currently the world's highest energy colliding beam facility. Its counter-rotating proton and antiproton beams collide at 2 TeV center-of-mass. Delivery of such intense beam fluxes to experiments has required improved knowledge of the Tevatron's beam optical lattice. An oscillating dipole magnet, referred to as an AC dipole, is one of such a tool to non-destructively assess the optical properties of the synchrotron. We discusses development of an AC dipole system for the Tevatron, a fast-oscillating (f ~ 20 kHz) dipole magnet which can be adiabatically turned on and off to establish sustained coherent oscillations of the beam particles without affecting the transverse emittance. By utilizing an existing magnet and a higher power audio amplifier, the cost of the Tevatron AC dipole system became relatively inexpensive. We discuss corrections which must be applied to the driven oscillation measurements to obtain the proper interpretation of beam optical parameters from AC dipole studies. After successful operations of the Tevatron AC dipole system, AC dipole systems, similar to that in the Tevatron, will be build for the CERN LHC. We present several measurements of linear optical parameters (beta function and phase advance) for the Tevatron, as well as studies of non-linear perturbations from sextupole and octupole elements.

  13. QCD at the Tevatron: Jets and fragmentation

    Energy Technology Data Exchange (ETDEWEB)

    V. Daniel Elvira

    2001-09-27

    At the Fermilab Tevatron energies, ({radical} s=1800 GeV and {radical} s = 630 GeV), jet production is the dominant process. During the period 1992-1996, the D0 and CDF experiments accumulated almost 100 pb{sup -1} of data and performed the most accurate jet production measurements up to this date. These measurements and the NLO-QCD theoretical predictions calculated during the last decade, have improved our understanding of QCD, our knowledge of the proton structure, and pushed the limit to the scale associated with quark compositeness to 2.4-2.7 TeV. In this paper, we present the most recent published and preliminary measurements on jet production and fragmentation by the D0 and CDF collaborations.

  14. Scientific Opportunity: the Tevatron and the LHC

    CERN Multimedia

    2010-01-01

    The press makes much of the competition between CERN’s LHC and Fermilab’s Tevatron in the search for the Higgs boson. This competitive aspect is real, and probably adds spice to the scientific exploration, but for us such reporting often feels like spilling the entire pepper shaker over a fine meal. The media’s emphasis on competition obscures the more important substance of our long-standing collaboration in scientific discovery.   Our laboratories and our communities have worked together for decades. Europeans have contributed greatly to the Tevatron’s many successes, including the discovery of the top quark, the discovery of fast oscillations in the decay of strange B mesons and the many searches for new phenomena. Americans have contributed to many programs at CERN, notably the extraordinary precision measurements of LEP, and more recently construction of the LHC accelerator and detectors. Fermilab scientists played a vital role throughout 2009 in...

  15. Neutrino results from the Fermilab Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Shaevitz, M.H. [Columbia Univ., New York, NY (United States); Arroyo, C. [Columbia Univ., New York, NY (United States); Bachmann, K.T. [Columbia Univ., New York, NY (United States); Bazarko, A.O. [Columbia Univ., New York, NY (United States); Blair, R.E. [Columbia Univ., New York, NY (United States); Bolton, T.A. [Columbia Univ., New York, NY (United States); Foudas, C. [Columbia Univ., New York, NY (United States); King, B.J. [Columbia Univ., New York, NY (United States); Lefmann, W.C. [Columbia Univ., New York, NY (United States); Leung, W.C. [Columbia Univ., New York, NY (United States); Mishra, S.R. [Columbia Univ., New York, NY (United States); Oltman, E. [Columbia Univ., New York, NY (United States); Quintas, P.Z. [Columbia Univ., New York, NY (United States); Rabinowitz, S.A. [Columbia Univ., New York, NY (United States); Sciulli, F. [Columbia Univ., New York, NY (United States); Seligman, W.G. [Columbia Univ., New York, NY (United States); Merritt, F.S. [University of Chicago, Chicago, IL 60637 (United States); Oreglia, M.J. [University of Chicago, Chicago, IL 60637 (United States); Schumm, B.A. [University of Chicago, Chicago, IL 60637 (United States); Bernstein, R.H. [Fermilab, Batavia, IL 60510 (United States); Borcherding, F. [Fermilab, Batavia, IL 60510 (United States); Fisk, H.E. [Fermilab, Batavia, IL 60510 (United States); Lamm, M.J. [Fermilab, Batavia, IL 60510 (United States); Marsh, W. [Fermilab, Batavia, IL 60510 (United States); Merritt, K.W.B. [Fermilab, Batavia, IL 60510 (United States); Schellman, H. [Fermilab, Batavia, IL 60510 (United States); Yovanovitch, D.D. [Fermilab, Batavia, IL 60510 (United States); Bodek, A. [University of Rochester, Rochester, NY 14627 (United States); Budd, H.S. [University of Rochester, Rochester, NY 14627 (United States); De Barbaro, P.; Salcumoto, W.K. [University of Rochester, Rochester, NY 14627 (United States)

    1995-01-01

    Results from the high-energy, high-statistics studies of neutrino nucleon interactions by the CCFR collaboration at the Fermilab Tevatron are described. Using a data sample of over 3.7million events with energies up to 600GeV, precision measurements are presented for the weak mixing angle, sin{sup 2}{theta}{sub w}, the structure functions, F{sub 2}(x,Q{sup 2}) and xF{sub 3}(x,Q{sup 2}), aud the strange quark distribution, xs(x,Q{sup 2}). Comparisons of these measurements to those obtained in other processes are made in the context of global electroweak and QCD tests. Prospects for the next generation measurements by the NuTeV collaboration at Fermilab are also presented. ((orig.)).

  16. Fixed target experiments at the Fermilab Tevatron

    CERN Document Server

    Gutierrez, Gaston

    2014-01-01

    This paper presents a review of the study of Exclusive Central Production at a Center of Mass energy of $\\sqrt{s}=40$ GeV at the Fermilab Fixed Target program. In all reactions reviewed in this paper, protons with an energy of 800 GeV were extracted from the Tevatron accelerator at Fermilab and directed to a Liquid Hydrogen target. The states reviewed include $\\pi^+\\pi^-$, $K^0_s K^0_s$, $ K^0_sK^\\pm\\pi^\\mp$, $\\phi\\phi$ and $D^{*\\pm}$. Partial Wave Analysis results will be presented on the light states but only the cross section will be reviewed in the diffractive production of $D^{*\\pm}$

  17. Top Quark Physics at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Jung, Andreas W. [Fermi National Accelerator Lab. (FNAL), Batavia, IL (United States). Particle Physics Division

    2015-05-21

    An overview of recent top quark measurements using the full Run II data set of CDF or D0 at the Tevatron is presented. Results are complementary to the ones at the LHC. Recent measurements of the production cross section of top quarks in strong and electroweak production and of top quark production asymmetries are presented. The latter includes the measurement of the tt-bar production asymmetry by D0 in the dilepton decay channel. Within their uncertainties the results from all these measurements agree with their respective Standard Model expectation. Finally latest updates on measurements of the top quark mass are discussed, which at the time of the conference are the most precise determinations.

  18. Du fratinoj

    Institute of Scientific and Technical Information of China (English)

    1996-01-01

    Vivis iam du fratinoj-Aje kaj Fatme.Iliapatrino estis duon-patrino por Fatme kaj in neamis.Foje i diris al sia edzo:-Faru kion ajn,sed mi ne plu volas vidiFatme.La sekvan tagon la patro forkondukis la

  19. Perturbative QCD tests from the LEP, HERA, and TEVATRON colliders

    Energy Technology Data Exchange (ETDEWEB)

    Kuhlmann, S. [Argonne National Lab., IL (United States)

    1994-09-01

    A review of QCD tests from LEP, HERA and the TEVATRON colliders is presented. This includes jet production, quark/gluon jet separation, quark/gluon propagator spin, {alpha}{sub s} updates, photon production, and rapidity gap experiments.

  20. Higgs boson studies at the Tevatron

    Science.gov (United States)

    Aaltonen, T.; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Agnew, J. P.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J. A.; Arisawa, T.; Artikov, A.; Asaadi, J.; Ashmanskas, W.; Askew, A.; Atkins, S.; Auerbach, B.; Augsten, K.; Aurisano, A.; Avila, C.; Azfar, F.; Badaud, F.; Badgett, W.; Bae, T.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barbaro-Galtieri, A.; Barberis, E.; Baringer, P.; Barnes, V. E.; Barnett, B. A.; Barria, P.; Bartlett, J. F.; Bartos, P.; Bassler, U.; Bauce, M.; Bazterra, V.; Bean, A.; Bedeschi, F.; Begalli, M.; Behari, S.; Bellantoni, L.; Bellettini, G.; Bellinger, J.; Benjamin, D.; Beretvas, A.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bhat, P. C.; Bhatia, S.; Bhatnagar, V.; Bhatti, A.; Bland, K. R.; Blazey, G.; Blessing, S.; Bloom, K.; Blumenfeld, B.; Bocci, A.; Bodek, A.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bortoletto, D.; Boudreau, J.; Boveia, A.; Brandt, A.; Brandt, O.; Brigliadori, L.; Brock, R.; Bromberg, C.; Bross, A.; Brown, D.; Brucken, E.; Budagov, J.; Bu, X. B.; Budd, H. S.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Burkett, K.; Busetto, G.; Bussey, P.; Buszello, C. P.; Butti, P.; Buzatu, A.; Calamba, A.; Camacho-Pérez, E.; Camarda, S.; Campanelli, M.; Canelli, F.; Carls, B.; Carlsmith, D.; Carosi, R.; Carrillo, S.; Casal, B.; Casarsa, M.; Casey, B. C. K.; Castilla-Valdez, H.; Castro, A.; Catastini, P.; Caughron, S.; Cauz, D.; Cavaliere, V.; Cavalli-Sforza, M.; Cerri, A.; Cerrito, L.; Chakrabarti, S.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Chen, Y. C.; Chertok, M.; Chiarelli, G.; Chlachidze, G.; Cho, K.; Cho, S. W.; Choi, S.; Chokheli, D.; Choudhary, B.; Cihangir, S.; Ciocci, M. A.; Claes, D.; Clark, A.; Clarke, C.; Clutter, J.; Convery, M. E.; Conway, J.; Cooke, M.; Cooper, W. E.; Corbo, M.; Corcoran, M.; Cordelli, M.; Couderc, F.; Cousinou, M.-C.; Cox, C. A.; Cox, D. J.; Cremonesi, M.; Cruz, D.; Cuevas, J.; Culbertson, R.; Cutts, D.; d'Ascenzo, N.; Das, A.; Datta, M.; Davies, G.; De Barbaro, P.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demina, R.; Demortier, L.; Deninno, M.; Denisov, D.; Denisov, S. P.; d'Errico, M.; Desai, S.; Deterre, C.; DeVaughan, K.; Devoto, F.; Di Canto, A.; Di Ruzza, B.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dittmann, J. R.; Dominguez, A.; Donati, S.; D'Onofrio, M.; Dorigo, M.; Driutti, A.; Dubey, A.; Dudko, L. V.; Duperrin, A.; Dutt, S.; Eads, M.; Ebina, K.; Edgar, R.; Edmunds, D.; Elagin, A.; Ellison, J.; Elvira, V. D.; Enari, Y.; Erbacher, R.; Errede, S.; Esham, B.; Eusebi, R.; Evans, H.; Evdokimov, V. N.; Facini, G.; Farrington, S.; Fauré, A.; Feng, L.; Ferbel, T.; Fernández Ramos, J. P.; Fiedler, F.; Field, R.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Flanagan, G.; Forrest, R.; Fortner, M.; Fox, H.; Franklin, M.; Freeman, J. C.; Frisch, H.; Fuess, S.; Funakoshi, Y.; Garcia-Bellido, A.; García-González, J. A.; Garfinkel, A. F.; Garosi, P.; Gavrilov, V.; Geng, W.; Gerber, C. E.; Gerberich, H.; Gerchtein, E.; Gershtein, Y.; Giagu, S.; Giakoumopoulou, V.; Gibson, K.; Ginsburg, C. M.; Ginther, G.; Giokaris, N.; Giromini, P.; Giurgiu, G.; Glagolev, V.; Glenzinski, D.; Gold, M.; Goldin, D.; Golossanov, A.; Golovanov, G.; Gomez, G.; Gomez-Ceballos, G.; Goncharov, M.; González López, O.; Gorelov, I.; Goshaw, A. T.; Goulianos, K.; Gramellini, E.; Grannis, P. D.; Greder, S.; Greenlee, H.; Grenier, G.; Grinstein, S.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grosso-Pilcher, C.; Group, R. C.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Guimaraes da Costa, J.; Gutierrez, G.; Gutierrez, P.; Hahn, S. R.; Haley, J.; Han, J. Y.; Han, L.; Happacher, F.; Hara, K.; Harder, K.; Hare, M.; Harel, A.; Harr, R. F.; Harrington-Taber, T.; Hatakeyama, K.; Hauptman, J. M.; Hays, C.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinrich, J.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herndon, M.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hocker, A.; Hoeneisen, B.; Hogan, J.; Hohlfeld, M.; Holzbauer, J. L.; Hong, Z.; Hopkins, W.; Hou, S.; Howley, I.; Hubacek, Z.; Hughes, R. E.; Husemann, U.; Hussein, M.; Huston, J.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Introzzi, G.; Iori, M.; Ito, A. S.; Ivanov, A.; Jabeen, S.; Jaffré, M.; James, E.; Jang, D.; Jayasinghe, A.; Jayatilaka, B.; Jeon, E. J.; Jeong, M. S.; Jesik, R.; Jiang, P.; Jindariani, S.; Johns, K.; Johnson, E.; Johnson, M.; Jonckheere, A.; Jones, M.; Jonsson, P.; Joo, K. K.; Joshi, J.; Jun, S. Y.; Jung, A. W.; Junk, T. R.; Juste, A.; Kajfasz, E.; Kambeitz, M.; Kamon, T.; Karchin, P. E.; Karmanov, D.; Kasmi, A.; Kato, Y.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Ketchum, W.; Keung, J.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kilminster, B.; Kim, D. H.; Kim, H. S.; Kim, J. E.; Kim, M. J.; Kim, S. B.; Kim, S. H.; Kim, Y. J.; Kim, Y. K.; Kimura, N.; Kirby, M.; Kiselevich, I.; Knoepfel, K.; Kohli, J. M.; Kondo, K.; Kong, D. J.; Konigsberg, J.; Kotwal, A. V.; Kozelov, A. V.; Kraus, J.; Kreps, M.; Kroll, J.; Kruse, M.; Kuhr, T.; Kumar, A.; Kupco, A.; Kurata, M.; Kurča, T.; Kuzmin, V. A.; Laasanen, A. T.; Lammel, S.; Lammers, S.; Lancaster, M.; Lannon, K.; Latino, G.; Lebrun, P.; Lee, H. S.; Lee, H. S.; Lee, J. S.; Lee, S. W.; Lee, W. M.; Lei, X.; Lellouch, J.; Leo, S.; Leone, S.; Lewis, J. D.; Li, D.; Li, H.; Li, L.; Li, Q. Z.; Lim, J. K.; Limosani, A.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipeles, E.; Lipton, R.; Lister, A.; Liu, H.; Liu, H.; Liu, Q.; Liu, T.; Liu, Y.; Lobodenko, A.; Lockwitz, S.; Loginov, A.; Lokajicek, M.; Lopes de Sa, R.; Lucchesi, D.; Lueck, J.; Lujan, P.; Lukens, P.; Luna-Garcia, R.; Lungu, G.; Lyon, A. L.; Lys, J.; Lysak, R.; Maciel, A. K. A.; Madar, R.; Madrak, R.; Maestro, P.; Magaña-Villalba, R.; Malik, S.; Malik, S.; Malyshev, V. L.; Manca, G.; Manousakis-Katsikakis, A.; Mansour, J.; Margaroli, F.; Marino, P.; Martínez, M.; Martínez-Ortega, J.; Matera, K.; Mattson, M. E.; Mazzacane, A.; Mazzanti, P.; McCarthy, R.; McGivern, C. L.; McNulty, R.; Mehta, A.; Mehtala, P.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Mesropian, C.; Meyer, A.; Meyer, J.; Miao, T.; Miconi, F.; Mietlicki, D.; Mitra, A.; Miyake, H.; Moed, S.; Moggi, N.; Mondal, N. K.; Moon, C. S.; Moore, R.; Morello, M. J.; Mukherjee, A.; Mulhearn, M.; Muller, Th.; Murat, P.; Mussini, M.; Nachtman, J.; Nagai, Y.; Naganoma, J.; Nagy, E.; Nakano, I.; Napier, A.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Nett, J.; Neu, C.; Neustroev, P.; Nguyen, H. T.; Nigmanov, T.; Nodulman, L.; Noh, S. Y.; Norniella, O.; Nunnemann, T.; Oakes, L.; Oh, S. H.; Oh, Y. D.; Oksuzian, I.; Okusawa, T.; Orava, R.; Orduna, J.; Ortolan, L.; Osman, N.; Osta, J.; Pagliarone, C.; Pal, A.; Palencia, E.; Palni, P.; Papadimitriou, V.; Parashar, N.; Parihar, V.; Park, S. K.; Parker, W.; Partridge, R.; Parua, N.; Patwa, A.; Pauletta, G.; Paulini, M.; Paus, C.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Phillips, T. J.; Piacentino, G.; Pianori, E.; Pilot, J.; Pitts, K.; Plager, C.; Pleier, M.-A.; Podstavkov, V. M.; Pondrom, L.; Popov, A. V.; Poprocki, S.; Potamianos, K.; Pranko, A.; Prewitt, M.; Price, D.; Prokopenko, N.; Prokoshin, F.; Ptohos, F.; Punzi, G.; Qian, J.; Quadt, A.; Quinn, B.; Ranjan, N.; Ratoff, P. N.; Razumov, I.; Redondo Fernández, I.; Renton, P.; Rescigno, M.; Rimondi, F.; Ripp-Baudot, I.; Ristori, L.; Rizatdinova, F.; Robson, A.; Rodriguez, T.; Rolli, S.; Rominsky, M.; Ronzani, M.; Roser, R.; Rosner, J. L.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Ruffini, F.; Ruiz, A.; Russ, J.; Rusu, V.; Sajot, G.; Sakumoto, W. K.; Sakurai, Y.; Sánchez-Hernández, A.; Sanders, M. P.; Santi, L.; Santos, A. S.; Sato, K.; Savage, G.; Saveliev, V.; Savoy-Navarro, A.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schlabach, P.; Schmidt, E. E.; Schwanenberger, C.; Schwarz, T.; Schwienhorst, R.; Scodellaro, L.; Scuri, F.; Seidel, S.; Seiya, Y.; Sekaric, J.; Semenov, A.; Severini, H.; Sforza, F.; Shabalina, E.; Shalhout, S. Z.; Shary, V.; Shaw, S.; Shchukin, A. A.; Shears, T.; Shepard, P. F.; Shimojima, M.; Shochet, M.; Shreyber-Tecker, I.; Simak, V.; Simonenko, A.; Sinervo, P.; Skubic, P.; Slattery, P.; Sliwa, K.; Smirnov, D.; Smith, J. R.; Snider, F. D.; Snow, G. R.; Snow, J.; Snyder, S.; Söldner-Rembold, S.; Song, H.; Sonnenschein, L.; Sorin, V.; Soustruznik, K.; Stancari, M.; St. Denis, R.; Stark, J.; Stelzer, B.; Stelzer-Chilton, O.; Stentz, D.; Stoyanova, D. A.; Strauss, M.; Strologas, J.; Sudo, Y.; Sukhanov, A.; Suslov, I.; Suter, L.; Svoisky, P.; Takemasa, K.; Takeuchi, Y.; Tang, J.; Tecchio, M.; Teng, P. K.; Thom, J.; Thomson, E.; Thukral, V.; Titov, M.; Toback, D.; Tokar, S.; Tokmenin, V. V.; Tollefson, K.; Tomura, T.; Tonelli, D.; Torre, S.; Torretta, D.; Totaro, P.; Trovato, M.; Tsai, Y.-T.; Tsybychev, D.; Tuchming, B.; Tully, C.; Ukegawa, F.; Uozumi, S.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Van Kooten, R.; van Leeuwen, W. M.; Varelas, N.; Varnes, E. W.; Vasilyev, I. A.; Vázquez, F.; Velev, G.; Vellidis, C.; Verkheev, A. Y.; Vernieri, C.; Vertogradov, L. S.; Verzocchi, M.; Vesterinen, M.; Vidal, M.; Vilanova, D.; Vilar, R.; Vizán, J.; Vogel, M.; Vokac, P.; Volpi, G.; Wagner, P.; Wahl, H. D.; Wallny, R.; Wang, S. M.; Wang, M. H. L. S.; Wang, R.-J.; Warburton, A.; Warchol, J.; Waters, D.; Watts, G.; Wayne, M.; Weichert, J.; Welty-Rieger, L.; Wester, W. C., III; Whiteson, D.; Wicklund, A. B.; Wilbur, S.; Williams, H. H.; Williams, M. R. J.; Wilson, G. W.; Wilson, J. S.; Wilson, P.; Winer, B. L.; Wittich, P.; Wobisch, M.; Wolbers, S.; Wolfe, H.; Wood, D. R.; Wright, T.; Wu, X.; Wu, Z.; Wyatt, T. R.; Xie, Y.; Yamada, R.; Yamamoto, K.; Yamato, D.; Yang, S.; Yang, T.; Yang, U. K.; Yang, Y. C.; Yao, W.-M.; Yasuda, T.; Yatsunenko, Y. A.; Ye, W.; Ye, Z.; Yeh, G. P.; Yi, K.; Yin, H.; Yip, K.; Yoh, J.; Yorita, K.; Yoshida, T.; Youn, S. W.; Yu, G. B.; Yu, I.; Yu, J. M.; Zanetti, A.; Zeng, Y.; Zennamo, J.; Zhao, T. G.; Zhou, B.; Zhou, C.; Zhu, J.; Zielinski, M.; Zieminska, D.; Zivkovic, L.; Zucchelli, S.

    2013-09-01

    We combine searches by the CDF and D0 Collaborations for the standard model Higgs boson with mass in the range 90-200GeV/c2 produced in the gluon-gluon fusion, WH, ZH, tt¯H, and vector boson fusion processes, and decaying in the H→bb¯, H→W+W-, H→ZZ, H→τ+τ-, and H→γγ modes. The data correspond to integrated luminosities of up to 10fb-1 and were collected at the Fermilab Tevatron in pp¯ collisions at s=1.96TeV. The searches are also interpreted in the context of fermiophobic and fourth generation models. We observe a significant excess of events in the mass range between 115 and 140GeV/c2. The local significance corresponds to 3.0 standard deviations at mH=125GeV/c2, consistent with the mass of the Higgs boson observed at the LHC, and we expect a local significance of 1.9 standard deviations. We separately combine searches for H→bb¯, H→W+W-, H→τ+τ-, and H→γγ. The observed signal strengths in all channels are consistent with the presence of a standard model Higgs boson with a mass of 125GeV/c2.

  1. Higgs Boson Studies at the Tevatron

    CERN Document Server

    Aaltonen, T.; Abbott, B.; Acharya, B.S.; Adams, M.; Adams, T.; Alexeev, G.D.; Alkhazov, G.; Alton, A.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J.A.; Arisawa, T.; Artikov, A.; Asaadi, J.; Ashmanskas, W.; Askew, A.; Atkins, S.; Auerbach, B.; Augsten, K.; Aurisano, A.; Avila, C.; Azfar, F.; Badaud, F.; Badgett, W.; Bae, T.; Bagby, L.; Baldin, B.; Bandurin, D.V.; Banerjee, S.; Barbaro-Galtieri, A.; Barberis, E.; Baringer, P.; Barnes, V.E.; Barnett, B.A.; Barria, P.; Bartlett, J.F.; Bartos, P.; Bassler, U.; Bauce, M.; Bazterra, V.; Bean, A.; Bedeschi, F.; Begalli, M.; Behari, S.; Bellantoni, L.; Bellettini, G.; Bellinger, J.; Benjamin, D.; Beretvas, A.; Beri, S.B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besancon, M.; Beuselinck, R.; Bhat, P.C.; Bhatia, S.; Bhatnagar, V.; Bhatti, A.; Bland, K.R.; Blazey, G.; Blessing, S.; Bloom, K.; Blumenfeld, B.; Bocci, A.; Bodek, A.; Boehnlein, A.; Boline, D.; Boos, E.E.; Borissov, G.; Bortoletto, D.; Boudreau, J.; Boveia, A.; Brandt, A.; Brandt, O.; Brigliadori, L.; Brock, R.; Bromberg, C.; Bross, A.; Brown, D.; Brucken, E.; Budagov, J.; Bu, X.B.; Budd, H.S.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Burkett, K.; Busetto, G.; Bussey, P.; Buszello, C.P.; Butti, P.; Buzatu, A.; Calamba, A.; Camacho-Perez, E.; Camarda, S.; Campanelli, M.; Canelli, F.; Carls, B.; Carlsmith, D.; Carosi, R.; Carrillo, S.; Casal, B.; Casarsa, M.; Casey, B.C.K.; Castilla-Valdez, H.; Castro, A.; Catastini, P.; Caughron, S.; Cauz, D.; Cavaliere, V.; Cavalli-Sforza, M.; Cerri, A.; Cerrito, L.; Chakrabarti, S.; Chakraborty, D.; Chan, K.M.; Chandra, A.; Chapon, E.; Chen, G.; Chen, Y.C.; Chertok, M.; Chiarelli, G.; Chlachidze, G.; Cho, K.; Cho, S.W.; Choi, S.; Chokheli, D.; Choudhary, B.; Cihangir, S.; Ciocci, M.A.; Claes, D.; Clark, A.; Clarke, C.; Clutter, J.; Convery, M.E.; Conway, J.; Cooke, M.; Cooper, W.E.; Corbo, M.; Corcoran, M.; Cordelli, M.; Couderc, F.; Cousinou, M.C.; Cox, C.A.; Cox, D.J.; Cremonesi, M.; Cruz, D.; Cuevas, J.; Culbertson, R.; Cutts, D.; d'Ascenzo, N.; Das, A.; Datta, M.; Davies, G.; de Barbaro, P.; de Jong, S., J.; De La Cruz-Burelo, E.; Deliot, F.; Demina, R.; Demortier, L.; Deninno, M.; Denisov, D.; Denisov, S.P.; d'Errico, M.; Desai, S.; Deterre, C.; DeVaughan, K.; Devoto, F.; Di Canto, A.; Di Ruzza, B.; Diehl, H.T.; Diesburg, M.; Ding, P.F.; Dittmann, J.R.; Dominguez, A.; Donati, S.; D'Onofrio, M.; Dorigo, M.; Driutti, A.; Dubey, A.; Dudko, L.V.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Ebina, K.; Edgar, R.; Edmunds, D.; Elagin, A.; Ellison, J.; Elvira, V.D.; Enari, Y.; Erbacher, R.; Errede, S.; Esham, B.; Eusebi, R.; Evans, H.; Evdokimov, V.N.; Facini, G.; Farrington, S.; Faure, A.; Feng, L.; Ferbel, T.; Fernandez Ramos, J.P.; Fiedler, F.; Field, R.; Filthaut, F.; Fisher, W.; Fisk, H.E.; Flanagan, G.; Forrest, R.; Fortner, M.; Fox, H.; Franklin, M.; Freeman, J.C.; Frisch, H.; Fuess, S.; Funakoshi, Y.; Garcia-Bellido, A.; Garcia-Gonzalez, J.A.; Garcia-Guerra, G.A.; Garfinkel, A.F.; Garosi, P.; Gavrilov, V.; Geng, W.; Gerber, C.E.; Gerberich, H.; Gerchtein, E.; Giagu, S.; Giakoumopoulou, V.; Gibson, K.; Ginsburg, C.M.; Ginther, G.; Giokaris, N.; Giromini, P.; Giurgiu, G.; Glagolev, V.; Glenzinski, D.; Gold, M.; Goldin, D.; Golossanov, A.; Golovanov, G.; Gomez, G.; Gomez-Ceballos, G.; Goncharov, M.; Gonzalez Lopez, O.; Gorelov, I.; Goshaw, A.T.; Goulianos, K.; Gramellini, E.; Grannis, P.D.; Greder, S.; Greenlee, H.; Grenier, G.; Grinstein, S.; Gris, Ph.; Grivaz, J.F.; Grohsjean, A.; Grosso-Pilcher, C.; Group, R.C.; Grunendahl, S.; Grunewald, M.W.; Guillemin, T.; Guimaraes da Costa, J.; Gutierrez, G.; Gutierrez, P.; Hahn, S.R.; Haley, J.; Han, J.Y.; Han, L.; Happacher, F.; Hara, K.; Harder, K.; Hare, M.; Harel, A.; Harr, R.F.; Harrington-Taber, T.; Hatakeyama, K.; Hauptman, J.M.; Hays, C.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinrich, J.; Heinson, A.P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herndon, M.; Herner, K.; Hesketh, G.; Hildreth, M.D.; Hirosky, R.; Hoang, T.; Hobbs, J.D.; Hocker, A.; Hoeneisen, B.; Hogan, J.; Hohlfeld, M.; Hong, Z.; Hopkins, W.; Hou, S.; Howley, I.; Hubacek, Z.; Hughes, R.E.; Husemann, U.; Hussein, M.; Huston, J.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Introzzi, G.; Iori, M.; Ito, A.S.; Ivanov, A.; Jabeen, S.; Jaffre, M.; James, E.; Jang, D.; Jayasinghe, A.; Jayatilaka, B.; Jeon, E.J.; Jeong, M.S.; Jesik, R.; Jiang, P.; Jindariani, S.; Johns, K.; Johnson, E.; Johnson, M.; Jonckheere, A.; Jones, M.; Jonsson, P.; Joo, K.K.; Joshi, J.; Jun, S.Y.; Jung, A.W.; Junk, T.R.; Juste, A.; Kajfasz, E.; Kambeitz, M.; Kamon, T.; Karchin, P.E.; Karmanov, D.; Kasmi, A.; Kato, Y.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Ketchum, W.; Keung, J.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y.N.; Kilminster, B.; Kim, D.H.; Kim, H.S.; Kim, J.E.; Kim, M.J.; Kim, S.B.; Kim, S.H.; Kim, Y.J.; Kim, Y.K.; Kimura, N.; Kirby, M.; Kiselevich, I.; Knoepfel, K.; Kohli, J.M.; Kondo, K.; Kong, D.J.; Konigsberg, J.; Kotwal, A.V.; Kozelov, A.V.; Kraus, J.; Kreps, M.; Kroll, J.; Kruse, M.; Kuhr, T.; Kumar, A.; Kupco, A.; Kurata, M.; Kurca, T.; Kuzmin, V.A.; Laasanen, A.T.; Lammel, S.; Lammers, S.; Lancaster, M.; Lannon, K.; Latino, G.; Lebrun, P.; Lee, Hyeon-Seung; Lee, Hyun Su; Lee, J.S.; Lee, S.W.; Lee, W.M.; Lei, X.; Lellouch, J.; Leo, S.; Leone, S.; Lewis, J.D.; Li, D.; Li, D.; Li, H.; Li, L.; Li, Q.Z.; Lim, J.K.; Limosani, A.; Lincoln, D.; Linnemann, J.; Lipaev, V.V.; Lipeles, E.; Lipton, R.; Lister, A.; Liu, H.; Liu, H.; Liu, Q.; Liu, T.; Liu, Y.; Lobodenko, A.; Lockwitz, S.; Loginov, A.; Lokajicek, M.; Lopes de Sa, R.; Lucchesi, D.; Lueck, J.; Lujan, P.; Lukens, P.; Luna-Garcia, R.; Lungu, G.; Lyon, A.L.; Lys, J.; Lysak, R.; Maciel, A.K.A.; Madar, R.; Madrak, R.; Maestro, P.; Magana-Villalba, R.; Malik, S.; Malik, S.; Malyshev, V.L.; Manca, G.; Manousakis-Katsikakis, A.; Mansour, J.; Margaroli, F.; Marino, P.; Martinez, M.; Martinez-Ortega, J.; Matera, K.; Mattson, M.E.; Mazzacane, A.; Mazzanti, P.; McCarthy, R.; McGivern, C.L.; McNulty, R.; Mehta, A.; Mehtala, P.; Meijer, M.M.; Melnitchouk, A.; Menezes, D.; Mercadante, P.G.; Merkin, M.; Mesropian, C.; Meyer, A.; Meyer, J.; Miao, T.; Miconi, F.; Mietlicki, D.; Mitra, A.; Miyake, H.; Moed, S.; Moggi, N.; Mondal, N.K.; Moon, C.S.; Moore, R.; Morello, M.J.; Mukherjee, A.; Mulhearn, M.; Muller, Th.; Murat, P.; Mussini, M.; Nachtman, J.; Nagai, Y.; Naganoma, J.; Nagy, E.; Naimuddin, M.; Nakano, I.; Napier, A.; Narain, M.; Nayyar, R.; Neal, H.A.; Negret, J.P.; Nett, J.; Neu, C.; Neustroev, P.; Nguyen, H.T.; Nigmanov, T.; Nodulman, L.; Noh, S.Y.; Norniella, O.; Nunnemann, T.; Oakes, L.; Oh, S.H.; Oh, Y.D.; Oksuzian, I.; Okusawa, T.; Orava, R.; Orduna, J.; Ortolan, L.; Osman, N.; Osta, J.; Padilla, M.; Pagliarone, C.; Pal, A.; Palencia, E.; Palni, P.; Papadimitriou, V.; Parashar, N.; Parihar, V.; Park, S.K.; Parker, W.; Partridge, R.; Parua, N.; Patwa, A.; Pauletta, G.; Paulini, M.; Paus, C.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Petroff, P.; Phillips, T.J.; Piacentino, G.; Pianori, E.; Pilot, J.; Pitts, K.; Plager, C.; Pleier, M.A.; Podesta-Lerma, P.L.M.; Podstavkov, V.M.; Pondrom, L.; Popov, A.V.; Poprocki, S.; Potamianos, K.; Pranko, A.; Prewitt, M.; Price, D.; Prokopenko, N.; Prokoshin, F.; Ptohos, F.; Punzi, G.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M.S.; Ranjan, N.; Ratoff, P.N.; Razumov, I.; Redondo Fernandez, I.; Renton, P.; Rescigno, M.; Rimondi, F.; Ripp-Baudot, I.; Ristori, L.; Rizatdinova, F.; Robson, A.; Rodriguez, T.; Rolli, S.; Rominsky, M.; Ronzani, M.; Roser, R.; Rosner, J.L.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Ruffini, F.; Ruiz, A.; Russ, J.; Rusu, V.; Sajot, G.; Sakumoto, W.K.; Sakurai, Y.; Salcido, P.; Sanchez-Hernandez, A.; Sanders, M.P.; Santi, L.; Santos, A.S.; Sato, K.; Savage, G.; Saveliev, V.; Savoy-Navarro, A.; Sawyer, L.; Scanlon, T.; Schamberger, R.D.; Scheglov, Y.; Schellman, H.; Schlabach, P.; Schmidt, E.E.; Schwanenberger, C.; Schwarz, T.; Schwienhorst, R.; Scodellaro, L.; Scuri, F.; Seidel, S.; Seiya, Y.; Sekaric, J.; Semenov, A.; Severini, H.; Sforza, F.; Shabalina, E.; Shalhout, S.Z.; Shary, V.; Shaw, S.; Shchukin, A.A.; Shears, T.; Shepard, P.F.; Shimojima, M.; Shivpuri, R.K.; Shochet, M.; Shreyber-Tecker, I.; Simak, V.; Simonenko, A.; Sinervo, P.; Skubic, P.; Slattery, P.; Sliwa, K.; Smirnov, D.; Smith, J.R.; Smith, K.J.; Snider, F.D.; Snow, G.R.; Snow, J.; Snyder, S.; Soldner-Rembold, S.; Song, H.; Sonnenschein, L.; Sorin, V.; Soustruznik, K.; Stancari, M.; St. Denis, R.; Stark, J.; Stelzer, B.; Stelzer-Chilton, O.; Stentz, D.; Stoyanova, D.A.; Strauss, M.; Strologas, J.; Sudo, Y.; Sukhanov, A.; Suslov, I.; Suter, L.; Svoisky, P.; Takemasa, K.; Takeuchi, Y.; Tang, J.; Tecchio, M.; Teng, P.K.; Thom, J.; Thomson, E.; Thukral, V.; Titov, M.; Toback, D.; Tokar, S.; Tokmenin, V.V.; Tollefson, K.; Tomura, T.; Tonelli, D.; Torre, S.; Torretta, D.; Totaro, P.; Trovato, M.; Tsai, Y.T.; Tsybychev, D.; Tuchming, B.; Tully, C.; Ukegawa, F.; Uozumi, S.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Van Kooten, R.; Van Leeuwen, W.M.; Varelas, N.; Varnes, E.W.; Vasilyev, I.A.; Vazquez, F.; Velev, G.; Vellidis, C.; Verkheev, A.Y.; Vernieri, C.; Vertogradov, L.S.; Verzocchi, M.; Vesterinen, M.; Vidal, M.; Vilanova, D.; Vilar, R.; Vizan, J.; Vogel, M.; Vokac, P.; Volpi, G.; Wagner, P.; Wahl, H.D.; Wallny, R.; Wang, S.M.; Wang, M.H.L.S.; Wang, R.J.; Warburton, A.; Warchol, J.; Waters, D.; Watts, G.; Wayne, M.; Weichert, J.; Welty-Rieger, L.; Wester, W.C., III; White, A.; Whiteson, D.; Wicke, D.; Wicklund, A.B.; Wilbur, S.; Williams, H.H.; Williams, M.R.J.; Wilson, G.W.; Wilson, J.S.; Wilson, P.; Winer, B.L.; Wittich, P.; Wobisch, M.; Wolbers, S.; Wolfe, H.; Wood, D.R.; Wright, T.; Wu, X.; Wu, Z.; Wyatt, T.R.; Xie, Y.; Yamada, R.; Yamamoto, K.; Yamato, D.; Yang, S.; Yang, T.; Yang, U.K.; Yang, Y.C.; Yao, W.M.; Yasuda, T.; Yatsunenko, Y.A.; Ye, W.; Ye, Z.; Yeh, G.P.; Yi, K.; Yin, H.; Yip, K.; Yoh, J.; Yorita, K.; Yoshida, T.; Youn, S.W.; Yu, G.B.; Yu, I.; Yu, J.M.; Zanetti, A.; Zeng, Y.; Zennamo, J.; Zhao, T.G.; Zhou, B.; Zhou, C.; Zhu, J.; Zielinski, M.; Zieminska, D.; Zivkovic, L.; Zucchelli, S.

    2013-01-01

    We combine searches by the CDF and D0 Collaborations for the standard model Higgs boson with mass in the range 90--200 GeV/c^2 produced in the gluon-gluon fusion, WH, ZH, ttbarH, and vector boson fusion processes, and decaying in the H->bbbar, H->W^+W^-, H->ZZ, H->\\tau^+\\tau^-, and H->\\gamma \\gamma\\ modes. The data correspond to integrated luminosities of up to 10 fb^-1 and were collected at the Fermilab Tevatron in ppbar collisions at sqrt(s)=1.96 TeV. The searches are also interpreted in the context of fermiophobic and fourth generation models. We observe a significant excess of events in the mass range between 115 and 140 GeV/c^2. The local significance corresponds to 3.1 standard deviations at m_H=125 GeV/c^2, consistent with the mass of the Higgs boson observed at the LHC. Furthermore, we separately combine searches for H->bbbar, H->W^+W^-, H->\\tau^+\\tau^-, and H->\\gamma \\gamma. The observed signal strengths in all channels are consistent with the presence of a standard model Higgs boson with a mass of 1...

  2. Tevatron bunch length studies at CDF

    Energy Technology Data Exchange (ETDEWEB)

    Matthew Jones; Bob Kephart; and Rick Vidal

    2002-05-29

    A luminous interaction region can be described by the distribution in (x, y, z) over which p{bar p} interactions are observed in a detector. The spatial size of this distribution can be written in terms of expressions that involve only combinations of the proton and anti-proton bunch sizes. Hence, it is not possible to determine the sizes of the proton and anti-proton bunches independently by fitting the distribution of (x, y, z) from the recorded events. If, in addition to the coordinates (x, y, z) at which p{bar p} interactions occur, the times at which the interactions took place are also measured, then it becomes possible to measure the lengths of the proton and anti-proton bunches separately. This sensitivity is due to a correlation between z and t that arises from the fact that the proton and anti-proton bunches travel in opposite directions. The derivation presented in section 2 quantifies this correlation, resulting in an expression for the probability density as a function of z and t for p{bar p} interactions. By fitting the distributions observed at CDF using this model, we measure the lengths of the proton and anti-proton bunches at times throughout several Tevatron stores. From this analysis the evolution of the bunch lengths can be studied. We attempt to correlate these with other measures of the bunch length obtained using different experimental techniques.

  3. Updated overview of the Tevatron control system

    Energy Technology Data Exchange (ETDEWEB)

    Lucas, P.

    1987-10-01

    A single unified control system is used for all of the Fermilab accelerators and storage rings, from the LINAC to the Tevatron and antiproton source. A review of the general features is given - these include a 'host' system consisting of a number of minicomputers integrated with many distributed microprocessors in a variety of subsystems, usage of an in-house developed protocol, GAS, for communication between the two classes of machines, and a Parameter Page program, designed in conjunction with the system database, which allows a wide variety of quantities to be read and set in a coherent fashion. Recent developments include the implementation of a block transfer and 'fast time plot' facility through CAMAC, inclusion of several new computers in the host, a better understanding of system throughput, greatly improved reliability, advent of programs which sequence a large number of independent operations, and the construction of new hardware subsystems. Possible future system upgrades will be briefly presented. A summary of the utilization of a quite large software staff, at a time when the system is no longer under construction, will be discussed.

  4. La maquette digitale du tunnel du LEP

    CERN Document Server

    Brouns, G

    2000-01-01

    Pour l'installation du LHC et son équipement périphérique (ligne cryogénique, câbles, tuyauterie, etc.) dans le tunnel du LEP, une maquette digitale CAO doit être faite. Après un rappel de la définition théorique du tunnel du LEP, cette LHC project Note décrit comment sont utilisées et intégrées d'anciennes et de nouvelles mesures du tunnel pour arriver à un ensemble de données qui permettent de construire la maquette digitale (CAO) du tunnel du LHC. Ensuite, les résultats sont comparés à leur valeur théorique d'une part, et aux anciennes valeurs disponibles d'autre part.

  5. Tevatron-for-LHC Report of the QCD Working Group

    Energy Technology Data Exchange (ETDEWEB)

    Albrow, Michael G.; Begel, M.; Bourilkov, D.; Campanelli, M.; Chlebana, F.; De Roeck, A.; Dittmann, J.R.; Ellis, S.D.; Field, B.; Field, R.; Gallinaro, M.; /Fermilab

    2006-10-01

    The experiments at Run 2 of the Tevatron have each accumulated over 1 fb{sup -1} of high-transverse momentum data. Such a dataset allows for the first precision (i.e. comparisons between theory and experiment at the few percent level) tests of QCD at a hadron collider. While the Large Hadron Collider has been designed as a discovery machine, basic QCD analyses will still need to be performed to understand the working environment. The Tevatron-for-LHC workshop was conceived as a communication link to pass on the expertise of the Tevatron and to test new analysis ideas coming from the LHC community. The TeV4LHC QCD Working Group focused on important aspects of QCD at hadron colliders: jet definitions, extraction and use of Parton Distribution Functions, the underlying event, Monte Carlo tunes, and diffractive physics. This report summarizes some of the results achieved during this workshop.

  6. Le transfert de connaissances entre les mathematiques et les sciences. Une etude exploratoire aupres d'eleves de 4e secondaire

    Science.gov (United States)

    Samson, Ghislain

    2003-06-01

    Au moment ou dans plusieurs pays on travaille a refondre les programmes d'etudes, tant au primaire qu'au secondaire, l'interet pour le transfert renait. Un des concepts fondamentaux en apprentissage consiste en l'habilete a reutiliser de facon consciente et efficace un acquis d'une situation a une autre situation. Cette recherche emane de preoccupations professionnelles au moment ou le chercheur etait enseignant au secondaire. Au cours de ces annees, il lui a ete possible de constater que plusieurs eleves percevaient difficilement les liens presents entre les disciplines mathematiques et scientifiques. Des travaux en psychologie cognitive et plus particulierement selon une perspective du traitement de l'information ont servi de cadre de reference pour evaluer et analyser les capacites de transfert aupres d'eleves de 4e secondaire. Ce cadre de reference permet de formuler le principal objectif qui est de mieux comprendre le processus de transfert chez des eleves en situation de resolution de problemes scientifiques. Cette these s'interesse donc au transfert en tant que phenomene important du processus d'apprentissage au sens de l'integration. La methode de recherche choisie, de nature qualitative, est principalement axee sur l'evaluation de la capacite a transferer des connaissances lors d'une epreuve et d'un entretien. Pour evaluer ce potentiel de transfert, nous avons elabore deux outils: une epreuve en mathematiques et en sciences et un guide d'entretien. Pour la passation de l'epreuve, le chercheur a pu compter sur la collaboration de 130 sujets provenant de deux ecoles. L'entretien complete la prise de donnees avec 13 sujets ayant accepte de poursuivre l'etude. Les donnees recueillies par ces instruments font ensuite l'objet d'une analyse de contenu. En premier lieu, les verbatims de l'epreuve et de l'entretien ont ete transcrits, puis codifies. La correction des reponses fournies pour les problemes resolus s'est faite a partir d'une grille d

  7. Searches for the standard model Higgs boson at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Dorigo, Tommaso; /Padua U.

    2005-05-01

    The CDF and D0 experiments at the Tevatron have searched for the Standard Model Higgs boson in data collected between 2001 and 2004. Upper limits have been placed on the production cross section times branching ratio to b{bar b} pairs or W{sup +}W{sup -} pairs as a function of the Higgs boson mass. projections indicate that the Tevatron experiments have a chance of discovering a M{sub H} = 115 GeV Higgs with the total dataset foreseen by 2009, or excluding it at 95% C.L. up to a mass of 135 GeV.

  8. Legacy limits and hints of New Physics at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Duperrin, Arnaud; /Marseille, CPPM

    2011-12-01

    This paper reviews results of beyond-the-standard model searches at the Tevatron presented in a plenary talk at the Europhysics Conference on High Energy Physics (EPS-HEP) in Grenoble. Here I present a selection of results from the CDF and D0 experiments that were shown at the conference during the parallel sessions. Much more is available and can be found at the experiment's web pages. This proceeding essentially focuses on searches in the dilepton, diboson, and t{bar t} final states. Throughout the paper, hints of new physics observed at the Tevatron are also briefly discussed.

  9. A fast injection kicker system for the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Chris C. Jensen, Robert E. Reilly and Bruce M. Hanna

    2001-07-25

    A new proton injection kicker system is required for the Tevatron in the Run II era. The new system was designed to supply 1.25 kG-m into a magnetic aperture of 48 mm vertical x 71 mm horizontal x 5 m long with a 396 ns bunch spacing. The system was designed to be upgraded to 132 ns bunch spacing with additional pulse supplies. The system design tradeoffs needed to meet these goals is discussed. These include the system topology, the system impedance and the number of magnets. This system has been installed in the Tevatron.

  10. Searches for Beyond SM Higgs Boson at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Safonov, A.; /Texas A-M

    2006-05-01

    In the following, the authors describe preliminary results of searches for non-SM higgs bosons at the CDF and D0 experiments. Both experiments use data obtained in p{bar p} collisions at the Tevatron at {radical}s = 1.96 TeV.

  11. Searches for Standard Model Higgs at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Cortavitarte, Rocio Vilar; /Cantabria Inst. of Phys.

    2007-11-01

    A summary of the latest results of Standard Model Higgs boson searches from CDF and D0 presented at the DIS 2007 conference is reported in this paper. All analyses presented use 1 fb{sup -1} of Tevatron data. The strategy of the different analyses is determined by the Higgs production mechanism and decay channel.

  12. Searches for standard model Higgs at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Vilar Cortabitarte, Rocio; /Cantabria U., Santander

    2007-04-01

    A summary of the latest results of Standard Model Higgs boson searches from CDF and D0 presented at the DIS 2007 conference is reported in this paper. All analyses presented use 1 fb{sup -1} of Tevatron data. The strategy of the different analyses is determined by the Higgs production mechanism and decay channel.

  13. High pt jets and photons at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Gerber, Cecilia E.; /Illinois U., Chicago

    2005-09-01

    The authors present recent results on high p{sub T} jets and photon production in {bar p}p collisions at a center of mass energy of 1.96 TeV. The measurements were performed by the CDF and D0 collaborations using between 150 and 300 pb{sup -1} of data taken during Run II at the Tevatron.

  14. Tevatron Top $A_{FB}$ Versus LHC Top Physics

    CERN Document Server

    Gresham, Moira I; Zurek, Kathryn M

    2011-01-01

    We carry out a comprehensive analysis of models for top A_{FB} at the Tevatron in light of new top data arriving from the LHC. We begin with a careful Tevatron analysis, considering in general which sets of effective vertices give rise to a large forward-backward asymmetry while suppressing the contribution to the total t\\bar{t} cross-section. We show on general grounds that scalar models struggle to produce sufficient asymmetries, while vector models can produce a large asymmetry with a less significant tension in the total cross-section and t\\bar{t} invariant mass distribution at the Tevatron. We examine the essential observables of these models for top physics at LHC7 with 1 fb^{-1} of data, including the total cross-section, invariant mass distribution and number of additional jets in t\\bar{t} events. In the case of t-channel mediators, the LHC total cross-section places a strong constraint on light mediators, while the Tevatron invariant mass distributions place strong constraints on heavy mediators that...

  15. Race for the Higgs hots up as Tevatron seeks extension

    CERN Multimedia

    Banks, Michael

    2009-01-01

    "With researchers at Cern's Large Hadron Collider (LHC) having circulated protons for the first time since last year's accident, the US Department of Energy (DOE) is requesting $25m so that the Tevatron collider at the Fermi National Accelerator Laboratory in Illinois can run for an extra year until 2011" (0.25 page)

  16. Neutrino production of dimuons at the Fermilab Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Shaevitz, M.H.; Arroyo, C.; Bachmann, K.T.; Bazarko, A.O.; Blair, R.E.; Bolton, T.; Foudis, C.; King, B.J.; Lefmann, W.C.; Leung, W.C.; Mishra, S.R.; Oltman, E.; Quintas, P.Z.; Rabinowitz, S.A.; Sciulli, F.; Seligman, W.G. (Columbia University, New York, NY 10027 (United States)); Merritt, F.S.; Oreglia, M.J.; Schumm, B.A. (University of Chicago, Chicago, IL 60637 (United States)); Bernstein, R.H.; Borcherding, F.; Fisk, H.E.; Lamm, M.J.; Marsh, W.; Merritt, K.W.B.; Schellman, H.; Yovanovitch, D.D. (Fermilab, Batavia, IL 60510 (United States)); Bodek, A.; Budd, H.S.; de Barbaro, P.; Sakamuto, W.K. (University of Rochester, Rochester, NY 14627 (United States)); Smith, W.H.; Kinnel, T.S.; Sandler, P.H. (University of Wisconsin, Madison, WI 53706 (United States))

    1992-02-01

    Neutrino and antineutrino interactions with two muons in the final state have been studied by the CCFR collaboration in the Fermilab Tevatron neutrino beam. The rate of neutrino- and antineutrino-induced prompt same-sign dimuon production in steel was measured using a sample of 220 [mu][sup [minus

  17. Enhancing the top signal at Tevatron using Neural Nets

    CERN Document Server

    Ametller, L; Talavera, P; Ll Ametller; Ll Garrido

    1994-01-01

    We show that Neural Nets can be useful for top analysis at Tevatron. The main features of t\\bar t and background events on a mixed sample are projected in a single output, which controls the efficiency and purity of the t\\bar t signal.

  18. Electroweak Theory for the Tevatron, LHC, and ILC

    CERN Document Server

    Erler, Jens

    2008-01-01

    Future high precision electroweak measurements require understanding of Standard Model expectations to multi-loop accuracy, both, for the predictions of production cross-sections of signal and background, as well as for pseudo-observables. I review recent results from precision calculations and summarize projections and implications for the Tevatron, the LHC, CEBAF, and the ILC.

  19. Review of Physics Results from the Tevatron: Heavy Flavor Physics

    CERN Document Server

    Lewis, Jonathan

    2014-01-01

    We present a review of heavy flavor physics results from the CDF and D0 Collaborations operating at the Fermilab Tevatron Collider. A summary of results from Run 1 is included, but we concentrate on legacy results of charm and $b$ physics from Run 2, including results up to Summer 2014.

  20. Review of Physics Results from the Tevatron: Heavy Flavor Physics

    OpenAIRE

    Lewis, Jonathan; Van Kooten, Rick

    2014-01-01

    Comment: References added; text tweaked. Article submitted to the International Journal of Modern Physics A (IJMPA) as one of the seven chapters of the special issue on the "Review of Physics at the Tevatron", editor G. Bernardi. This article contains the chapter on the heavy flavor physics part of the review. 53 pages, 32 figures, 276 references

  1. Les jeux vidéo compétitifs au prisme des jeux sportifs : du sport au sport électronique

    OpenAIRE

    Besombes, Nicolas

    2016-01-01

    La comparaison entre jeux vidéo compétitifs et jeux sportifs fait régulièrement débat, et ce notamment auprès des acteurs de la communauté du sport électronique. À l’aide de concepts empruntés à la sociologie du sport, l’article propose de questionner la définition du sport électronique au regard de quatre critères objectifs et opérationnels régulièrement utilisés pour définir le jeu sportif : la pertinence motrice de l’activité, l’organisation de compétitions, le système règlementaire et le ...

  2. Du logiciel libre pour l’Assemblée nationale : Liberté du code versus liberté des usages

    OpenAIRE

    Chibois, Jonathan

    2013-01-01

    International audience; Fin 2006, l’Assemblée nationale française choisi de doter pour la treizième législature de logiciels exclusivement libres les postes informatiques des bureaux parlementaires. Le récit de l’évolution du projet de sa conception jusqu’à sa réalisation, puis à son déploiement auprès des utilisateurs, illustre quelles attentes cette technologie a suscité durant la décennie 2000-2010, et donc les défis qui se sont imposés à eux. Le fait est que le projet n’a pas été à la hau...

  3. Yukawa correction to top-quark production at the Tevatron

    CERN Document Server

    Stange, A; Stange, Alan; Willenbrock, Scott

    1993-01-01

    We calculate the correction to $\\qbq\\to\\tbt$ of order $\\gmm$. This correction, proportional to the square of the Higgs-boson Yukawa coupling to the top quark, arises from loops of Higgs bosons and the scalar component of virtual vector bosons. The Yukawa correction to the total \\tbt\\ production cross section at the Fermilab Tevatron in the standard Higgs model is found to be much less than the theoretical uncertainty in the cross section. However, in a two-Higgs-doublet model, Yukawa couplings are generally enhanced. The Yukawa correction can increase the total $t\\bar t$ production cross section in this model by as much as $20$-$35\\%$, which is potentially observable at the Tevatron.

  4. Search for resonant second generation slepton production at the Tevatron

    CERN Document Server

    Abazov, V M; Abolins, M; Acharya, B S; Adams, M; Adams, T; Agelou, M; Agram, J L; Ahn, S H; Ahsan, M; Alexeev, G D; Alkhazov, G; Alton, A; Alverson, G; Alves, G A; Anastasoaie, M; Andeen, T; Anderson, S; Andrieu, B; Anzelc, M S; Arnoud, Y; Arov, M; Askew, A; Åsman, B; Assis-Jesus, A C S; Atramentov, O; Autermann, C; Avila, C; Ay, C; Badaud, F; Baden, A; Bagby, L; Baldin, B; Bandurin, D V; Banerjee, P; Banerjee, S; Barberis, E; Bargassa, P; Baringer, P; Barnes, C; Barreto, J; Bartlett, J F; Bassler, U; Bauer, D; Bean, A; Begalli, M; Begel, M; Belanger-Champagne, C; Bellantoni, L; Bellavance, A; Benítez, J A; Beri, S B; Bernardi, G; Bernhard, R; Berntzon, L; Bertram, I; Besançon, M; Beuselinck, R; Bezzubov, V A; Bhat, P C; Bhatnagar, V; Binder, M; Biscarat, C; Black, K M; Blackler, I; Blazey, G; Blekman, F; Blessing, S; Bloch, D; Bloom, K; Blumenschein, U; Böhnlein, A; Boeriu, O; Bolton, T A; Borcherding, F; Borissov, G; Bos, K; Bose, T; Brandt, A; Brock, R; Brooijmans, G; Bross, A; Brown, D; Buchanan, N J; Buchholz, D; Bühler, M; Büscher, V; Burdin, S; Burke, S; Burnett, T H; Busato, E; Buszello, C P; Butler, J M; Calfayan, P; Calvet, S; Cammin, J; Caron, S; Carvalho, W; Casey, B C K; Cason, N M; Castilla-Valdez, H; Chakrabarti, S; Chakraborty, D; Chan, K M; Chandra, A; Chapin, D; Charles, F; Cheu, E; Chevallier, F; Cho, D K; Choi, S; Choudhary, B; Christofek, L; Claes, D; Clement, B; Clément, C; Coadou, Y; Cooke, M; Cooper, W E; Coppage, D; Corcoran, M; Cousinou, M C; Cox, B; Crepe-Renaudin, S; Cutts, D; Cwiok, M; Da Motta, H; Das, A; Das, M; Davies, B; Davies, G; Davis, G A; De, K; de Jong, P; De Jong, S J; De La Cruz-Burelo, E; De Oliveira Martins, C; Degenhardt, J D; Déliot, F; Demarteau, M; Demina, R; Demine, P; Denisov, D; Denisov, S P; Desai, S; Diehl, H T; Diesburg, M; Doidge, M; Dominguez, A; Dong, H; Dudko, L V; Duflot, L; Dugad, S R; Duperrin, A; Dyer, J; Dyshkant, A; Eads, M; Edmunds, D; Edwards, T; Ellison, J; Elmsheuser, J; Elvira, V D; Eno, S; Ermolov, P; Estrada, J; Evans, H; Evdokimov, A; Evdokimov, V N; Fatakia, S N; Feligioni, L; Ferapontov, A V; Ferbel, T; Fiedler, F; Filthaut, F; Fisher, W; Fisk, H E; Fleck, I; Ford, M; Fortner, M; Fox, H; Fu, S; Fuess, S; Gadfort, T; Galea, C F; Gallas, E; Galyaev, E; García, C; García-Bellido, A; Gardner, J; Gavrilov, V; Gay, A; Gay, P; Gelé, D; Gelhaus, R; Gerber, C E; Gershtein, Yu; Gillberg, D; Ginther, G; Gollub, N; Gómez, B; Gounder, K; Goussiou, A; Grannis, P D; Greenlee, H; Greenwood, Z D; Gregores, E M; Grenier, G; Gris, P; Grivaz, J F; Grünendahl, S; Grünewald, M W; Guo, F; Guo, J; Gutíerrez, G; Gutíerrez, P; Haas, A; Hadley, N J; Haefner, P; Hagopian, S; Haley, J; Hall, I; Hall, R E; Han, L; Hanagaki, K; Harder, K; Harel, A; Harrington, R; Hauptman, J M; Hauser, R; Hays, J; Hebbeker, T; Hedin, D; Hegeman, J G; Heinmiller, J M; Heinson, A P; Heintz, U; Hensel, C; Hesketh, G; Hildreth, M D; Hirosky, R; Hobbs, J D; Hoeneisen, B; Hoeth, H; Hohlfeld, M; Hong, S J; Hooper, R; Houben, P; Hu, Y; Hubacek, Z; Hynek, V; Iashvili, I; Illingworth, R; Ito, A S; Jabeen, S; Jaffré, M; Jain, S; Jakobs, K; Jarvis, C; Jenkins, A; Jesik, R; Johns, K; Johnson, C; Johnson, M; Jonckheere, A; Jonsson, P; Juste, A; Käfer, D; Kahn, S; Kajfasz, E; Kalinin, A M; Kalk, J M; Kalk, J R; Kappler, S; Karmanov, D; Kasper, J; Kasper, P; Katsanos, I; Kau, D; Kaur, R; Kehoe, R; Kermiche, S; Kesisoglou, S; Khalatyan, N; Khanov, A; Kharchilava, A I; Kharzheev, Yu M; Khatidze, D; Kim, H; Kim, T J; Kirby, M H; Klima, B; Kohli, J M; Konrath, J P; Kopal, M; Korablev, V M; Kotcher, J; Kothari, B; Koubarovsky, A; Kozelov, A V; Kozminski, J; Kryemadhi, A; Krzywdzinski, S; Kühl, T; Kumar, A; Kunori, S; Kupco, A; Kurca, T; Kvita, J; Lager, S; Lammers, S; Landsberg, G L; Lazoflores, J; Le Bihan, A C; Lebrun, P; Lee, W M; Leflat, A; Lehner, F; Lesne, V; Lévêque, J; Lewis, P; Li, J; Li, Q Z; Lima, J G R; Lincoln, D; Linnemann, J; Lipaev, V V; Lipton, R; Liu, Z; Lobo, L; Lobodenko, A; Lokajícek, M; Lounis, A; Love, P; Lubatti, H J; Lynker, M; Lyon, A L; Maciel, A K A; Madaras, R J; Mättig, P; Magass, C; Magerkurth, A; Magnan, A M; Makovec, N; Mal, P K; Malbouisson, H B; Malik, S; Malyshev, V L; Mao, H S; Maravin, Y; Martens, M; Mattingly, S E K; McCarthy, R; McCroskey, R; Meder, D; Melnitchouk, A; Mendes, A; Mendoza, L; Merkin, M; Merritt, K W; Meyer, A; Meyer, J; Michaut, M; Miettinen, H; Millet, T; Mitrevski, J; Molina, J; Mondal, N K; Monk, J; Moore, R W; Moulik, T; Muanza, G S; Mulders, M; Mulhearn, M; Mundim, L; Mutaf, Y D; Nagy, E; Naimuddin, M; Narain, M; Naumann, N A; Neal, H A; Negret, J P; Nelson, S; Neustroev, P; Nöding, C; Nomerotski, A; Novaes, S F; Nunnemann, T; O'Dell, V; O'Neil, D C; Obrant, G; Oguri, V; Oliveira, N; Oshima, N; Otec, R; Oteroy-Garzon, G J; Owen, M; Padley, P; Parashar, N; Park, S J; Park, S K; Parsons, J; Partridge, R; Parua, N; Patwa, A; Pawloski, G; Perea, P M; Pérez, E; Peters, K; Petroff, P; Petteni, M; Piegaia, R; Pleier, M A; Podesta-Lerma, P L M; Podstavkov, V M; Pogorelov, Y; Pol, M E; Pompos, A; Pope, B G; Popov, A V; Prado da Silva, W L; Prosper, H B; Protopopescu, S D; Qian, J; Quadt, A; Quinn, B; Rani, K J; Ranjan, K; Rapidis, P A; Ratoff, P N; Renkel, P; Reucroft, S; Rijssenbeek, M; Ripp-Baudot, I; Rizatdinova, F K; Robinson, S; Rodrigues, R F; Royon, C; Rubinov, P; Ruchti, R; Rud, V I; Sajot, G; Sánchez-Hernández, A; Sanders, M P; Santoro, A F S; Savage, G; Sawyer, L; Scanlon, T; Schaile, A D; Schamberger, R D; Scheglov, Y; Schellman, H; Schieferdecker, P; Schmitt, C; Schwanenberger, C; Schwartzman, A; Schwienhorst, R; Sen-Gupta, S; Severini, H; Shabalina, E; Shamim, M; Shary, V; Shchukin, A A; Shephard, W D; Shivpuri, R K; Shpakov, D; Siccardi, V; Sidwell, R A; Simák, V; Sirotenko, V I; Skubic, P L; Slattery, P F; Smith, R P; Snow, G R; Snow, J; Snyder, S; Söldner-Rembold, S; Song, X; Sonnenschein, L; Sopczak, A; Sosebee, M; Soustruznik, K; Souza, M; Spurlock, B; Stark, J; Steele, J; Stevenson, K; Stolin, V; Stone, A; Stoyanova, D A; Strandberg, J; Strang, M A; Strauss, M; Ströhmer, R; Strom, D; Strovink, M; Stutte, L; Sumowidagdo, S; Sznajder, A; Talby, M; Tamburello, P; Taylor, W; Telford, P; Temple, J; Tiller, B; Titov, M; Tokmenin, V V; Tomoto, M; Toole, T; Torchiani, I; Towers, S; Trefzger, T; Trincaz-Duvoid, S; Tsybychev, D; Tuchming, B; Tully, C; Turcot, A S; Tuts, P M; Unalan, R; Uvarov, L; Uvarov, S; Uzunyan, S; Vachon, B; Vanden Berg, P J; Van Kooten, R; Van Leeuwen, W M; Varelas, N; Varnes, E W; Vartapetian, A H; Vasilyev, I A; Vaupel, M; Verdier, P; Vertogradov, L S; Verzocchi, M; Villeneuve-Séguier, F; Vint, P; Vlimant, J R; Von Törne, E; Voutilainen, M; Vreeswijk, M; Wahl, H D; Wang, L; Warchol, J; Watts, G; Wayne, M; Weber, M; Weerts, H; Wermes, N; Wetstein, M; White, A; Wicke, D; Wilson, G W; Wimpenny, S J; Wobisch, M; Womersley, J; Wood, D R; Wyatt, T R; Xie, Y; Xuan, N; Yacoob, S; Yamada, R; Yan, M; Yasuda, T; Yatsunenko, Y A; Yip, K; Yoo, H D; Youn, S W; Yu, C; Yu, J; Yurkewicz, A; Zatserklyaniy, A; Zeitnitz, C; Zhang, D; Zhao, T; Zhao, Z; Zhou, B; Zhu, J; Zielinski, M; Zieminska, D; Zieminski, A; Zutshi, V; Zverev, E G

    2006-01-01

    We present a search for supersymmetry in the R-parity violating resonant production and decay of smuons and muon-sneutrinos in the channels smuon->neutralino_1 muon, smuon->neutralino_2 muon, and muon-sneutrino->chargino muon. We analyzed 0.38 fb^-1 of integrated luminosity collected between April 2002 and August 2004 with the D0 detector at the Fermilab Tevatron Collider. The observed number of events is in agreement with the standard model expectation, and we calculate 95% C.L. limits on the slepton production cross section times branching fraction to gaugino plus muon, as a function of slepton and gaugino masses. In the framework of minimal supergravity, we set limits on the coupling parameter lambda'_211, extending significantly previous results obtained in Run I of the Tevatron and at the CERN LEP collider.

  5. BMSSM Higgs Bosons at the Tevatron and the LHC

    Energy Technology Data Exchange (ETDEWEB)

    Carena, Marcela; /Fermilab /Chicago U., EFI; Ponton, Eduardo; /Columbia U.; Zurita, Jose; /Zurich U.

    2010-05-01

    We study extensions of the Minimal Supersymmetric Standard Model (MSSM) with new degrees of freedom that couple sizably to the MSSM Higgs sector and lie in the TeV range. After integrating out the physics at the TeV scale, the resulting Higgs spectrum can significantly differ from typical supersymmetric scenarios, thereby providing a window Beyond the MSSM (BMSSM). Taking into account current LEP and Tevatron constraints, we perform an in-depth analysis of the Higgs collider phenomenology and explore distinctive characteristics of our scenario with respect to both the Standard Model and the MSSM. We propose benchmark scenarios to illustrate specific features of BMSSM Higgs searches at the Tevatron and the LHC.

  6. Searches for New Physics at the Tevatron and LHC

    Energy Technology Data Exchange (ETDEWEB)

    Wittich, Peter; /Cornell U., LEPP

    2011-11-01

    This is an auspicious moment in experimental particle physics - there are large data samples at the Tevatron and a new energy regime being explored at the Large Hadron Collider with ever larger data samples. The coincidence of these two events suggests that we will soon be able to address the question, what lies beyond the standard model? Particle physics's current understanding of the universe is embodied in it. The model has been tested to extreme precision - better than a part in ten thousand - but we suspect that it is only an approximation, and that physics beyond this standard model will appear in the data of the Tevatron and LHC in the near future. This brief review touches on the status of searches for new physics at the time of the conference.

  7. Synchrotron radiation based beam diagnostics at the Fermilab Tevatron

    CERN Document Server

    Thurman-Keup, R; Hahn, A; Hurh, P; Lorman, E; Lundberg, C; Meyer, T; Miller, D; Pordes, S; Valishev, A

    2011-01-01

    Synchrotron radiation has been used for many years as a beam diagnostic at electron accelerators. It is not normally associated with proton accelerators as the intensity of the radiation is too weak to make detection practical. However, if one utilizes the radiation originating near the edge of a bending magnet, or from a short magnet, the rapidly changing magnetic field serves to enhance the wavelengths shorter than the cutoff wavelength, which for more recent high energy proton accelerators such as Fermilab's Tevatron, tends to be visible light. This paper discusses the implementation at the Tevatron of two devices. A transverse beam profile monitor images the synchrotron radiation coming from the proton and antiproton beams separately and provides profile data for each bunch. A second monitor measures the low-level intensity of beam in the abort gaps which poses a danger to both the accelerator's superconducting magnets and the silicon detectors of the high energy physics experiments. Comparisons of measur...

  8. Selected Topics from Top Mass Measurements at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Schwienhorst, Reinhard [Michigan State U.

    2016-12-07

    The most recent results of the top-quark mass measurements at the Tevatron at Fermilab are presented. Data were collected in proton-antiproton collisions at sqrt{s}=1.96 TeV by the CDF and D0 experiments. Top quark mass measurements in the lepton+jets, dilepton and alljet final states as well as their combination and the extraction of the mass from the cross-section measurement are presented.

  9. Searches for physics beyond the Standard Model at the Tevatron

    Indian Academy of Sciences (India)

    Alberto Annovi; for the CDF and D0 Collaborations

    2012-10-01

    During the last 10 years, the Fermilab Tevatron has produced $p \\bar{p}$ collision at a centre-of-mass energy of 1.96 TeV that the CDF and DO Collaborations have scrutinized looking for new physics in a wide range of final states. Here, recent updates of new physics searches are reported using a data sample of up to 9 fb-1

  10. Top Quark Production Cross Section at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Shabalina, E.; /Chicago U.

    2006-05-01

    An overview of the preliminary results of the top quark pair production cross section measurements at a center-of-mass energy of 1.96 TeV carried out by the CDF and D0 collaborations is presented. The data samples used for the analyses are collected in the current Tevatron run and correspond to an integrated luminosity from 360 pb{sup -1} up to 760 pb{sup -1}.

  11. Searches for BSM (non-SUSY) physics at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Gerberich, Heather K.; /Illinois U., Urbana

    2005-11-01

    As of July 2005, the Tevatron at Fermilab has delivered {approx} 1 fb{sup -1} of data to the CDF and D0 experiments. Each experiment has recorded more than 80% of the delivered luminosity. Results of searches for physics (non-SUSY and non-Higgs) beyond the Standard Model using 200 pb{sup -1} to 480 pb{sup -1} at D0 and CDF are presented.

  12. Restoring the Skew Quadrupole Moment in Tevatron Dipoles

    CERN Document Server

    Harding, David J; Blowers, James N; Di Marco, Joseph; Glass, Henry; Hanft, Ray; John, Carson; Robotham, William; Tartaglia, M; Tompkins, John; Velev, Gueorgui

    2005-01-01

    In early 2003 it was realized that mechanical changes in the Tevatron dipoles had led to a deterioration of the magnetic field quality that was hindering operation of the accelerator. After extensive study, a remediation program was started in late 2003 which will continue through 2005. The mechanical and magnetic effects are discussed. The readjustment process and experience are reported, along with other observations on aging magnets.

  13. B-Physics at the Tevatron (Proceedings of PASCOS2010)

    OpenAIRE

    Ellison, John

    2010-01-01

    We report on recent B-Physics results from the Tevatron. The topics covered include measurement of the polarization amplitudes in $B_s^0 \\to \\phi \\phi$, the search for rare flavor-changing neutral-current decays, CP violation in $B_s^0 \\to J/\\psi \\phi$ and semileptonic $B_s^0$ decays, and a new measurement of the like-sign asymmetry in dimuon events.

  14. New Phenomena; 2, Recent Results from the Fermilab Tevatron

    CERN Document Server

    Toback, D

    2000-01-01

    The CDF and D\\O collaborations continue to search for new physics using more than 100~pb$^{-1}$ of \\xxbar{p} collisions at $\\sqrt{s}=1.8$ TeV collected at the Fermilab Tevatron. We present recent results from both experiments on R-parity violating Supersymmetry and $Z'$/Technicolor production with $ee$ and \\xxbar{t} final states. In addition we introduce Sherlock, a new quasi-model-independent search strategy.

  15. Review of Physics Results from the Tevatron: Top Quark Physics

    Energy Technology Data Exchange (ETDEWEB)

    Gerber, Cecilia E.; Vellidis, Costas

    2014-09-17

    We present results on top quark physics from the CDF and D0 collaborations at the Fermilab Tevatron proton anti-proton collider. These include legacy results from Run II that were published or submitted for publication before mid-2014, as well as a summary of Run I results. The historical perspective of the discovery of the top quark in Run I is also described.

  16. Neutrino production of dimuons at the Fermilab Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Smith, W.H.; Kinnel, T.S.; Sandler, P.H.; Arroyo, C.; Bachmann, K.T.; Bazarko, A.O.; Blair, R.E.; Foudas, C.; King, B.J.; Lefmann, W.C.; Leung, W.C.; Mishra, S.R.; Oltman, E.; Quintas, P.Z.; Rabinowitz, S.A.; Sciulli, F.; Seligman, W.G.; Shaevitz, M.H.; Merritt, F.S.; Oreglia, M.J.; Schumm, B.A.; Bernstein, R.H.; Borcherding, F.; Fisk, H.E.; Lamm, M.J.; Marsh, W.; Merritt, K.W.B.; Schellman, H.; Yovanovitch, D.D.; Bodek, A.; Budd, H.S.; Barbaro, P. de; Sakumoto, W.K. (Univ. of Wisconsin, Madison, WI (United States) Columbia Univ., New York, NY (United States) Univ. of Chicago, IL (United States) Fermilab, Batavia, IL (United States) Univ. of Rochester, NY (United States))

    1993-04-01

    Neutrino and antineutrino interactions with two muons in the final state have been studied by the CCFR collaboration in the Fermilab Tevatron neutrino beam. The rate of neutrino- and antineutrino-induced prompt same-sign dimuon production in steel was measured using a sample of 220 [mu][sup -] [mu][sup -] events and 15 [mu][sup +] [mu][sup +] events with P[sub [mu

  17. Tevatron-for-LHC Report: Preparations for Discoveries

    Energy Technology Data Exchange (ETDEWEB)

    Buescher, V.; Carena, Marcela S.; Dobrescu, Bogdan A.; Mrenna, S.; Rainwater, D.; Schmitt, M.

    2006-08-01

    This is the ''TeV4LHC'' report of the ''Physics Landscapes'' Working Group, focused on facilitating the start-up of physics explorations at the LHC by using the experience gained at the Tevatron. We present experimental and theoretical results that can be employed to probe various scenarios for physics beyond the Standard Model.

  18. OVERVIEW OF HIGGS BOSON STUDIES AT THE TEVATRON

    Energy Technology Data Exchange (ETDEWEB)

    Zivkovic, Lidija [Institute of Physics, Zemun, Serbia

    2014-05-01

    The CDF and D0 experiments at the Tevatron p¯p Collider collected data between 2002 and 2011, accumulating up to 10 fb-1 of data. During that time, an extensive search for the standard model Higgs boson was performed. Combined results from the searches for the standard model Higgs boson with the final dataset are presented, together with results on the Higgs boson couplings and spin and parity.

  19. Top quark pair production cross section at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Cortiana, Giorgio; /INFN, Padua /Padua U.

    2008-04-01

    Top quark pair production cross section has been measured at the Tevatron by CDF and D0 collaborations using different channels and methods, in order to test standard model predictions, and to search for new physics hints affecting the t{bar t} production mechanism or decay. Measurements are carried out with an integrated luminosity of 1.0 to 2.0 fb{sup -1}, and are found to be consistent with standard model expectations.

  20. Search for supersymmetric neutral Higgs bosons at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Scanlon, Tim; /Imperial Coll., London

    2007-10-01

    Recent preliminary results obtained by the CDF and D0 Collaborations on searches for Higgs bosons beyond the Standard Model at Run II of the Tevatron are discussed. The data, corresponding to integrated luminosities of up to 1 fb{sup -1}, are compared to theoretical expectations. No significant excess of signal above the expected background is observed in any of the various final states examined, and so limits at 95% Confidence Level (CL) are presented.

  1. Electromagnetic calorimeter and accurate measurement with the ATLAS detector of the LHC collider; Calorimetrie electromagnetique et mesures de precision avec le detecteur ATLAS aupres du collisionneur LHC

    Energy Technology Data Exchange (ETDEWEB)

    Pralavorio, P

    2007-06-15

    The main purpose of the ATLAS experiment is the understanding of the underlying mechanisms that drive the breaking of the electro-weak symmetry through the discovery of Higgs bosons. An important element to achieve this aim was the design of an electromagnetic calorimeter able to investigate the decay channels: H {yields} {gamma}{gamma} and H {yields} 4e. The high performance of the calorimeter will allow us to get a better accuracy on the measuring values of W and top masses which is essential to indirectly constrain the mass of the Higgs. In the same way, accurate measurements of top and W properties during the decays of top and tWb vertex will be necessary to question the standard model and to see beyond. The author has been working for 9 years in the ATLAS project, he has been involved in the design, construction, qualification and testing phases of the electromagnetic calorimeter of ATLAS. This document is a detailed presentation of the calorimeter, of its qualification and of its expectations when LHC is operating. This document is organized into 4 chapters: 1) assets and weaknesses of the standard model, 2) the ATLAS experiment, 3) the electromagnetic calorimeter, and 4) accurate measurements with ATLAS. This document presented before an academic board will allow its author to manage research works and particularly to tutor thesis students. (A.C.)

  2. Academic Training - Tevatron: studying pp collisions at the highest energy

    CERN Multimedia

    2006-01-01

    ACADEMIC TRAINING LECTURE SERIES 15, 16, 17, 18 May Main Auditorium, bldg. 500 on 15, 16, 17 May - Council Chamber on 18 May Physics at the Tevatron B. HEINEMANN, Univ. of Liverpool, FERMILAB Physics Results from the Tevatron The Tevatron proton-antiproton collider at Fermilab in the US is currently the world's highest energy collider. At the experiments CDF and D0 a broad physics programme is being pursued, ranging from flavour physics via electroweak precision measurements to searches for the Higgs boson and new particles beyond the Standard Model. In my lecture I will describe some of the highlight measurements in the flavour, electroweak and searches sectors, and the experimental techniques that are used. ENSEIGNEMENT ACADEMIQUE ACADEMIC TRAINING Françoise Benz 73127 academic.training@cern.ch If you wish to participate in one of the following courses, please tell to your supervisor and apply electronically from the course description pages that can be found on the Web at: http://www.cern.ch/...

  3. Présentation du volume

    Directory of Open Access Journals (Sweden)

    Ana Zwitter Vitez

    2012-12-01

    Full Text Available Dans de nombreuses disciplines scientifiques, le discours parlé représente depuis quelques décennies un objet de recherche proéminent. Ce fait s’explique probablement par deux caractéristiques principales du discours parlé: la structure complexe de sa matérialité et les fonctions variées de différentes pratiques langagières. C’est pourquoi le présent numéro réunit les articles basés sur les approches actuelles du discours parlé et sur les pratiques langagières spécifiques. Le volume est introduit par deux articles interdisciplinaires: Peter Garrard et Ahmed Samrah présentent le domaine de la pathologie du langage en donnant une revue fouillée sur les approches actuelles de l’analyse linguistique lors de la détection de la maladie d’Alzheimer, tandis que Harry Hollien donne un aperçu structuré sur le domaine de la phonétique judiciaire destiné à dévoiler l’identité des locuteurs et de détecter la déception dans le discours parlé. Les analyses explorant l’acquisition du langage commencent par l’article de Katharina Zipser qui examine la progression de structures grammaticales en les mettant en comparaison avec la compétence des apprenants et continuent par l’étude de Meta Lah proposant une évaluation des documents audiovisuels proposés aux apprenants de langue étrangère. Vesna Požgaj Hadži, Damir Horga et Tatjana Balažic Bulc remettent en question la corrélation entre la compétence linguistique et la fluence linguistique auprès de locuteurs non-maternels et l'analyse de Gemma Santiago Alonso aborde l'acquisition de l'article défini dans le langage enfantin. Les articles suivants se réunissent autour du domaine de l'interprétation: Jana Zidar Forte présente une approche actuelle dans l'entrainement d'interprètes, Lea Burjan analyse les phénomènes issus de la pratique de l'interprétation juridique et Simona  Šumrada traite de la reformulation dans le discours de la traduction et de

  4. Learning about Cri du Chat Syndrome

    Science.gov (United States)

    ... Learning About Prostate Cancer Learning About Cri du Chat Syndrome What is cri du chat syndrome? What ... cri du chat syndrome What is cri du chat syndrome? Cri du chat syndrome - also known as ...

  5. Breviaire du futur enseignant

    OpenAIRE

    Tarvydienė, Zita

    2003-01-01

    Mon expérience auprès des stagiaires montre que pour certains d’entre eux il reste souvent 5 ou 10 minutes inemployées avant la fin de la classe. Que font les étudiants? Certains demandent de faire des devoirs qui sont destinés à être faits à la maison; d’autres entament une nouvelle leçon. Bien sûr ce n’est pas bien car les apprenants n’ont plus d’énergie ni d’envie de travailler, leur concentration est dissipée, parfois le principe de la continuité est brisé. Au lieu de faire travailler ou ...

  6. 24 mars 2016 - Le Président de la Confédération suisse, Monsieur Johann Schneider-Ammann signe le livre d'or avec la Directrice générale du CERN Fabiola Gianotti.

    CERN Multimedia

    Brice, Maximilien

    2016-01-01

    Le Président de la Confédération suisse, Monsieur Johann Schneider-Ammann signe le livre d'or avec la Directrice générale du CERN Fabiola Gianotti. De g. à d.: F. Eder, Délégué aux Relations avec les Etats-hôtes; F. Bordry, Directeur des accélérateurs et de la technologie; S. E. M. l'Ambassadeur Fasel, Représentant permanent de la Suisse auprès de l’Office des Nations Unies et des autres organisations internationales à Genève; M. Steinacher, Directeur des finances et des ressources humaines et P. Pardo, Conseiller, Mission permanente de la Suisse auprès de l’Office des Nations Unies et des autres organisations internationales à Genève.

  7. Le Conseil du personnel, prêt pour les défis de 2015

    CERN Multimedia

    Association du personnel

    2015-01-01

    Afin de remplir d’une façon optimale sa mission de représentant du personnel CERN auprès de la Direction et des États membres, le Conseil du personnel s’appuie sur le travail d’un certain nombre de Commissions, parmi lesquelles conditions d’emploi, pensions, thèmes juridiques, protection sociale, hygiène et sécurité, InFormAction (formation, information et actions). Toutes ces commissions travaillent dans le but de contribuer à l’amélioration les conditions d’emploi des membres du personnel CERN. En particulier, dans le cadre de la préparation de l’examen quinquennal qui se terminera en décembre 2015 (5YR 2015). Rappelons que l’objet d’un examen quinquennal est d’assurer que les conditions financières et sociales offertes par l’Organisation lui permettent d&...

  8. Spectroscopy and Decay of $B$ Hadrons at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Paulini, Manfred

    2007-02-01

    The authors review recent results on heavy quark physics focusing on Run II measurements of B hadron spectroscopy and decay at the Tevatron. A wealth of new B physics measurements from CDF and D0 has been available. These include the spectroscopy of excited B states (B**, B**{sub s}) and the observation of the {Sigma}{sub b} baryon. The discussion of the decays of B hadrons and measurements of branching fractions focuses on charmless two-body decays of B {yields} h{sup +}h{sup -}. They report several new B{sub s}{sup 0} and {Lambda}{sub b}{sup 0} decay channels.

  9. B0(s) mixing studies at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Naimuddin, M.D.; /Delhi U.

    2006-05-01

    Measurement of the B{sub s}{sup 0} oscillation frequency via B{sub s}{sup 0} mixing analysis provides a powerful constraint on CKM matrix elements. This note briefly reviews the motivation behind these analyses and describes the various steps that go into a mixing measurement. Recent results on B{sub s}{sup 0} mixing obtained by the CDF and D0 collaborations using the data samples collected at Tevatron Collider in the period 2002-2005 are presented.

  10. Tevatron End-of-Run Beam Physics Experiments

    CERN Document Server

    Valishev, A; Miyamoto, R; White, S; Schmidt, F; Qiang, J

    2012-01-01

    Before the Tevatron Collider Run II ended in September of 2011, a number of specialized beam study periods were dedicated to the experiments on various accelerator physics concepts and effects during the last year of the machine operation. The study topics included collimation with bent crystals and hollow electron beams, diffusion measurements and various aspects of beambeam interactions. In this report we concentrate on the subject of beam-beam interactions, summarizing the results of beam experiments. The covered topics include offset collisions, coherent beam stability, effect of the bunch-length-to-beta-function ratio, and operation of AC dipole with colliding beams.

  11. Resonant second generation slepton production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Autermann, Christian Tobias [RWTH Aachen Univ. (Germany)

    2006-12-01

    A search for R-parity violating supersymmetry with the D0 detector at the Fermilab Tevatron p$\\bar{p}$-collider is presented. Assuming a non-zero LQ$\\bar{d}$ coupling λ$'\\atop{2jk}$ leads to final state with two muons and jets. A total integrated luminosity of 375 pb-1 collected between April 2002 and August 2004 is utilized. The observed number of events is in agreement with the Standard Model expectation, and limits on Rp supersymmetry are derived.

  12. Summary of Single top quark production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Schwienhorst, R. [Michigan State U.; CDF, on the

    2014-01-01

    The production of single-top quarks occurs via the weak interaction at the Fermilab Tevatron proton-antiproton collider. Single top quark events are selected in the lepton+jets final state by CDF and D0 and in the missing transverse energy plus jets final state by CDF. Multivariate classifiers separate the s-channel and t-channel single-top signals from the large backgrounds. The combination of CDF and D0 results leads to the first observation of the s-channel mode of single top quark production. The t-channel and single top combined cross sections have also been measured.

  13. Higgs boson production and properties at the Tevatron

    CERN Document Server

    Tuchming, Boris

    2014-01-01

    We present the searches for the Standard Model Higgs boson, using the full Run II dataset of the Fermilab Tevatron $p\\bar p$ collider, collected with the CDF and D\\O\\ detectors. A significant excess of events is observed, consistent with the presence of a Standard Model Higgs boson of mass 125 GeV. We also present tests of different spin/parity hypotheses, performed in the $VH \\to V b\\bar b$ channels at D\\O, and new searches in invisible modes conducted at CDF.

  14. Review of physics results from the Tevatron: QCD physics

    Energy Technology Data Exchange (ETDEWEB)

    Mesropian, Christina [Rockefeller U.; Bandurin, Dmitry [Virginia U.

    2015-02-17

    We present a summary of results from studies of quantum chromodynamics at the Fermilab Tevatron collider by the CDF and the D0 experiments. These include Run II results for the time period up to the end of Summer 2014. A brief description of Run I results is also given. This review covers a wide spectrum of topics, and includes measurements with jet and vector boson final states in the hard (perturbative) energy regime, as well as studies of soft physics such as diffractive and elastic scatterings, underlying and minimum bias events, hadron fragmentation, and multiple parton interactions.

  15. High Mass Standard Model Higgs searches at the Tevatron

    Directory of Open Access Journals (Sweden)

    Petridis Konstantinos A.

    2012-06-01

    Full Text Available We present the results of searches for the Standard Model Higgs boson decaying predominantly to W+W− pairs, at a center-of-mass energy of √s = 1.96 TeV, using up to 8.2 fb−1 of data collected with the CDF and D0 detectors at the Fermilab Tevatron collider. The analysis techniques and the various channels considered are discussed. These searches result in exclusions across the Higgs mass range of 156.5< mH <173.7 GeV for CDF and 161< mH <170 GeV for D0.

  16. Bottomonium Production at the Tevatron and the LHC

    CERN Document Server

    Domenech, J L

    2000-01-01

    Inclusive bottomonium hadroproduction at the Tevatron is firstly examined in a Monte Carlo framework with the colour-octet mechanism implemented in the event generation. We extract some NRQCD colour-octet matrix elements relevant for $\\Upsilon(1S)$ hadroproduction. Remarkably we find a quite small contribution (compatible with zero) from feeddown of $\\chi_{bJ}$ states produced through the colour-octet mechanism: $\\Upsilon(1S)$ indirect production via $\\chi_{bJ}$ decays should be mainly ascribed to the colour-singlet model. Finally we extrapolate to LHC energies to predict prompt $\\Upsilon(1S)$ production rates.

  17. E710, Proton, Antiproton Elastic Scattering at Tevatron Energies

    Science.gov (United States)

    Sadr, Sasan

    Experiment E710, located at site E0 of the Tevatron collider at Fermilab, was conceived in order to measure pp elastic scattering. The measured parameters were: the total cross section sigma_{t }, the ratio of the real to the imaginary part of the forward scattering amplitude rho, the nuclear slope parameter B, the nuclear curvature parameter C, the total elastic cross section sigma _{el}, and the single diffractive cross section sigma_{sd} . These measurements were taken at center-of-mass energies of sqrt{s}=1.02 and 1.8 TeV.

  18. LHC and Tevatron results on the tt differential cross sections

    CERN Document Server

    AUTHOR|(INSPIRE)INSPIRE-00213443; The ATLAS collaboration

    2017-01-01

    In this talk I will present a review of the most recent $t\\bar{t}$ differential cross sections measurement performed by LHC and Tevatron experiments. After a brief introduction, I will describe the mea- surements of fiducial and full phase-space differential cross sections based on events with exactly two, one or zero charged leptons in the final state. These results are compared to predictions made with Monte Carlo generators with next-to-leading order accuracy or next-to-next-to leading order numerical calculations.

  19. Low-Scale Technicolor at the Tevatron and LHC

    CERN Document Server

    Eichten, Estia

    2007-01-01

    The Tevatron experiments CDF and DO are close to making definitive statements about the technicolor discovery mode rho_T -> W pi_T for M(rho_T) gamma pi_T and l+l-, and a new one -- for the I^G J^{PC} = 1^- 1^{++} partner, a_T, of the rho_T. Adopting the argument that the technicolor contribution to S is reduced if M(a_T) is near M(rho_T), we enumerate important a_T decays and estimate production rates at the colliders.

  20. Searches for High Mass Resonances and Exotics at the Tevatron

    Directory of Open Access Journals (Sweden)

    Heintz Ulrich

    2012-06-01

    Full Text Available In this paper I review some recent searches for physics beyond the standard model from the CDF and D0 experiments at the Fermilab Tevatron collider based on an integrated luminosity of 5 to 7 fb−1 from pp¯ $par p$ collisions at 1.96 TeV. I present a selection of recent results from both the CDF and D0 collaborations covering searches for 4th generation t′ and b′ quarks, exotic resonances that decay to tt¯ $tar t$ quark pairs or ZZ boson pairs, universal extra dimensions, and dark matter particles.

  1. Le développement d'une qualité de coordination en EPS chez les élèves du CYT

    OpenAIRE

    Gremaud, Jessica; Favre, Romain; Weber, Serge

    2012-01-01

    La présente recherche porte sur l’enseignement de la qualité de coordination de différenciation en éducation physique et sportive (EPS) chez les élèves du cycle de transition. Elle a été conduite auprès de deux classes de 5ème année (8e année HarmoS). Ce travail propose dans un premier temps une approche théorique sur le déroulement du mouvement et sur la coordination motrice, puis une focalisation plus détaillée sur la qualité de différenciation. Elle présente et précise également le s...

  2. "Cirque du Freak."

    Science.gov (United States)

    Rivett, Miriam

    2002-01-01

    Considers the marketing strategies that underpin the success of the "Cirque du Freak" series. Describes how "Cirque du Freak" is an account of events in the life of schoolboy Darren Shan. Notes that it is another reworking of the vampire narrative, a sub-genre of horror writing that has proved highly popular with both adult and…

  3. Chlamydophilose abortive ovine : études à propos d'une suspicion de résistance de Chlamydophila abortus au vaccin vivant thermosensible dans des élevages ovins laitiers du rayon de Roquefort

    OpenAIRE

    Uhart, Maia

    2009-01-01

    Des cas d'avortements imputés à Chlamydophila abortus ont été décrits dans des élevages de brebis du rayon Roquefort (France, 12) alors que ces élevages pratiquaient la vaccination contre la chlamydophilose avec un vaccin vivant depuis plusieurs années. De brefs rappels bibliographiques concernant la chlamydophilose et la vaccination contre cette maladie sont présentés en première partie. Une enquête menée auprès de neuf éleveurs est ensuite exposée afin d'expliquer la persistance d'avortemen...

  4. Restaurant du Rivage, Vevey

    OpenAIRE

    Basini, Sari Bianca; Glocki, Ryszard Nikodem

    2015-01-01

    Après cinquante ans de mutilations, d'abandon et de spéculations économiques, le complexe du château de l'Aile et de la salle du Castillo à Vevey doit redéfinir son rôle public par rapport à la place du Marché et au Jardin du Rivage. S'appuyant sur la mémoire historique en ajoutant une unité à l'ensemble, nous créons un îlot regroupant des fonctions publiques. Il dessert ainsi l'espace ouvert environnant en articulant la relation entre le jardin et la place. L'élargissement de la promenade du...

  5. Aux membres du personnel français détachés au CERN - French version only

    CERN Multimedia

    2003-01-01

    Affiliation au régime de retraite français Le CERN a reçu la lettre suivante de la Mission permanente de la France auprès des Organisations Internationales à Genève au sujet de la récente publication d'un décret concernant la retraite des fonctionnaires français détachés dans les organisations internationales : " .. l'article 20 de la loi 2002-73 du 17 janvier 2002 a mis fin au caractère obligatoire de l'affiliation au régime de retraite français pour les fonctionnaires détachés à l'étranger ou dans les organisations internationales. Le décret 2002-1391 du 21 novembre 2002, publié au Journal Officiel du 28 novembre 2002, a prévu que les fonctionnaires concernés disposent d'un délai de quatre mois à partir de la notification de leur arrêté de détachement pour faire part à leur administration d'origine de leur volonté de continuer à cotiser au régime national. Pour les fonctionnaires ayant déjà reçu la notification de leur arrêté de détachement à la date du 1er décembre 20...

  6. In celebration of the fixed target program with the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Jeffrey A. Appel et al.

    2001-12-28

    The Tevatron is the world's first large superconducting accelerator. With its construction, we gained the dual opportunities to advance the state of the art in accelerator technology with the machine itself and in particle physics with the experiments that became possible in a higher energy regime. There have been 43 experiments in the Tevatron fixed target program. Many of these are better described as experimental programs, each with a broad range of physics goals and results, and more than 100 collaborating physicists and engineers. The results of this program are three-fold: (1) new technologies in accelerators, beams and detectors which advanced the state of the art; (2) new experimental results published in the refereed physics journals; and (3) newly trained scientists who are both the next generation of particle physicists and an important part of the scientific, technical and educational backbone of the country as a whole. In this book they compile these results. There are sections from each experiment including what their physics goals and results were, what papers were published, and which students have received degrees. Summaries of these results from the program as a whole are quite interesting, but the physics results from this program are too broad to summarize globally. The most important of the results appear in later sections of this booklet.

  7. A disoriented chiral condensate search at the Fermilab Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Convery, Mary Elizabeth [Case Western Reserve Univ., Cleveland, OH (United States)

    1997-05-01

    MiniMax (Fermilab T-864) was a small test/experiment at the Tevatron designed to search for disoriented chiral condensates (DCC) in the forward direction. Relativistic quantum field theory treats the vacuum as a medium, with bulk properties characterized by long-range order parameters. This has led to suggestions that regions of "disoriented vacuum" might be formed in high-energy collision processes. In particular, the approximate chiral symmetry of QCD could lead to regions of vacuum which have chiral order parameters disoriented to directions which have non-zero isospin, i.e. disoriented chiral condensates. A signature of DCC is the resulting distribution of the fraction of produced pions which are neutral. The MiniMax detector at the C0 collision region of the Tevatron was a telescope of 24 multi-wire proportional chambers (MWPC`s) with a lead converter behind the eighth MWPC, allowing the detection of charged particles and photon conversions in an acceptance approximately a circle of radius 0.6 in pseudorapidity-azimuthal-angle space, centered on pseudorapidity η ≈ 4. An electromagnetic calorimeter was located behind the MWPC telescope, and hadronic calorimeters and scintillator were located in the upstream anti-proton direction to tag diffractive events.

  8. A tevatron collider beauty factory. [Final report, 1980--1992

    Energy Technology Data Exchange (ETDEWEB)

    1992-12-31

    This document which is labeled a final report consists of several different items. The first is a proposal for a detector to be developed for beauty physics. The detector is proposed for the Fermilab Tevatron, and would be designed to measure mixing reactions, rare decay modes, and even CP violation in hadron collider beauty production. The general outline of the work proposed is given, and an estimate of the time to actually design the detector is presented, along with proposed changes to the Tevatron to accommodate the system. A preliminary report on an experiment to verify a reported observation of a 17 keV neutrino in tritium decay is presented. The present results in the decay spectra actually show a depression below expected levels, which is not consistent with a massive neutrino. Additional interest has been shown in finishing an electrostatic beta spectrometer which was started several years previously. The instrument uses hemispherical electrostatic electric fields to retard electrons emitted in tritium decay, allowing measurement of integral spectra. The design goal has a 5 eV energy resolution, which may be achievable. A new PhD student is pursuing this experiment. Also the report contains a proposal for additional work in the field of non-perturbative quantum field theory by the theoretical group at OU. The work which is proposed will be applied to electroweak and strong interactions, as well as to quantum gravitational phenomena.

  9. Searches for Low Mass Higgs Boson at the Tevatron

    Directory of Open Access Journals (Sweden)

    Sforza Federico

    2012-07-01

    Full Text Available We present the result of the searches for a low mass Standard Model Higgs boson performed at the Tevatron pp¯ $par p$ collider (√s = 1.96 TeV by the CDF and D0 experiments with an integrated luminosity of up to 8.5 fb-1. Individual searches are discussed and classified according to their sensitivity. Primary channels rely on the associate production with a vector boson (WH or ZH and the H → bb¯ $H o bar b$ decay channel (favored for MH ≲ 135 GeV/c2. Event selection is based on the leptonic decay of the vector boson and the identification of b–hadron enriched jets. Each individual channel is sensitive, for MH = 115 GeV/c2, to less than 5 times the SM expected cross section and the most sensitive channels can exclude a production cross section of 2.3×σHSM Secondary channels rely on a variety of final states. Although they are from 2 to 5 times less sensitive than any primary channel, they contribute to the Tevatron combination and, in some cases, they pose strong constrains on exotic Higgs boson models.

  10. Atlas du Liban

    Directory of Open Access Journals (Sweden)

    Ramez Philippe Maalouf

    2008-11-01

    Full Text Available Compte-rendu de l’ouvrage Atlas du Liban: territoires et société, sous la direction d’Éric Verdeil, Ghaleb Faour et Sébastien Velut, édition franco-libanaise de l’IFPO (Institut Français du Proche-Orient et du CNRS Liban (Conseil National de la Recherche Scientifique – Liban, Beyrouth 2007.Resenha do livro Atlas du Liban: territoires et société, sob a direção de Éric Verdeil, Ghaleb Faour e Sébastien Velut, editado por iniciativa franco-libanesa do IFPO (Institut Français du Proche-Orient e pelo CNRS Liban (Conseil National de la Recherche Scientifique – Liban, Beirute, 2007.Review of Atlas du Liban: territoires et société, edited by Éric Verdeil, Ghaleb Faour and Sébastien Velut, french-lebanese edition by IFPO (Institut Français du Proche-Orient and CNRS Liban (Conseil National de la Recherche Scientifique – Liban Beirut, 2007.

  11. Ecologie du phytoplancton du lac Kivu

    Directory of Open Access Journals (Sweden)

    Sarmento, H.

    2008-01-01

    Full Text Available Speciation within the African Coffee Pathogen. Cet article analyse s'il est avantageux d'utiliser le compost au lieu de l'engrais minéral pour produire la laitue dans la zone urbaine et péri-urbaine de Yaoundé. Les résultats de terrain montrent l'obtention de rendements et profits plus élevés lorsqu'on utilise le compost. Les résultats de la fonction de production Cobb-Douglas prouvent que l'utilisation du compost est statistiquement significative pour expliquer la variation de rendement de la laitue et que le compost est l'intrant le plus productif. D'autres résultats montrent que le compost fournit la matière organique utile au sol et que les besoins d'irrigation en eau de la culture sont réduits grâce à l'utilisation du compost. Par conséquent, malgré le fait que l'application du compost demande une main-d'oeuvre beaucoup plus élevée, son utilisation est généralement bénéfique pour les agriculteurs vivant aux alentours de Yaoundé. Les programmes de vulgarisation de cet intrant pour encourager son adoption devraient donc figurer parmi les points prioritaires dans la politique agricole du gouvernement camerounais.

  12. RÉSULTATS DE L’ENQUÊTE DE L’ASSOCIATION DU PERSONNEL AUPRÈS DU PERSONNEL : VOS PRIORITÉS

    CERN Multimedia

    Staff Association

    2014-01-01

    Cet article est le premier d’une série qui donnera plus de détails sur les résultats de l’enquête de l’Association du personnel réalisée auprès du personnel. Afin de connaitre vos priorités ainsi que l’évolution de vos préoccupations au cours de la dernière décennie, nous étudions comment, grâce à nos trois dernières enquêtes, vous avez choisi parmi une liste de 15 thèmes  les cinq plus importants, classés par ordre de priorité décroissant. Vous trouverez ci-dessous la liste des quinze thèmes accompagnés d’une description courte. L’évolution de la carrière (classification, niveau de recrutement, avancement, promotion) Le niveau de salaires La politique familial...

  13. Types du Caucase

    OpenAIRE

    Makhacheva, Taus

    2015-01-01

    Tiré du site Internet de Onestar Press: "Types du Caucase - antique postcard collection/ 2013 to the present time. Coming from the personal archive of the artist, these postcards date back to the 19th century and can be considered representative for the "popularized ethnography" of the Russian Empire. Their primitive typology follows the classical rules of exotization : they depict "pittoresque" groups from various tribes, families or nationalities, or representatives of diverse professions. ...

  14. Les outils du CERN

    CERN Multimedia

    1999-01-01

    C'est le plus grand centre mondial de recherche en physique des particules. Les outils du Laboratoire, accélérateurs et détecteurs de particules, figurent parmi les instruments scientifiques les plus complexes au monde. Des prix Nobels ont d'ailleurs été attribués aux physiciens du CERN pour leurs développements.

  15. New Measurements of Upsilon Spin Alignment at the Tevatron

    Directory of Open Access Journals (Sweden)

    Jones Matthew

    2012-06-01

    Full Text Available We describe a new analysis of γ(nS → μ+μ− decays collected in pp¯ $par p$ collisions with the CDF II detector at the Fermilab Tevatron. This analysis measures the angular distributions of the final state muons in the γ rest frame, providing new information about γ production polarization. We find the angular distributions to be nearly isotropic up to γ pT of 40 GeV/c, consistent with previous measurements by CDF, but inconsistent with results obtained by the D0 experiment. The results are compared with recent NLO calculations based on color-singlet matrix elements and non-relativistic QCD with color-octet matrix elements.

  16. Trilepton Signal of Grand Unified Models at the Tevatron

    CERN Document Server

    Accomando, E; Dutta, B

    2000-01-01

    At the Tevatron, the most promising channel to detect supersymmetry is three leptons plus missing energy, where the leptons are $e$'s and/or $\\mu$'s. This final state appears from the production of chargino and second lighetst neutralino. However in grand unified models with universal scalar masses at the grand unified scale, this final state mostly consists of $\\tau$'s which are hard to detect. We show that for some regions of non universality in the scalar masses at the GUT scale based on unifying groups like SU(5) or SO(10), the final state mostly consists of 3$l$+${\\rlap/E}_T$ and $\\tau ll$+${\\rlap/E}_T$. The first mode has very high detection efficiency and the second one is expected to have high detection efficency as well. We also show that these models can have enough events in these modes to be detected in RUN II.

  17. Search for quirks at the Fermilab Tevatron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Abazov, V.M.; /Dubna, JINR; Abbott, B.; /Oklahoma U.; Abolins, M.; /Michigan State U.; Acharya, B.S.; /Tata Inst.; Adams, M.; /Illinois U., Chicago; Adams, T.; /Florida State U.; Alexeev, G.D.; /Dubna, JINR; Alkhazov, G.; /St. Petersburg, INP; Alton, A.; /Augustana Coll., Sioux Falls /Michigan U.; Alverson, G.; /Northeastern U.; Alves, G.A.; /Rio de Janeiro, CBPF /NIKHEF, Amsterdam

    2010-08-01

    We report results of a search for particles with anomalously high ionization in events with a high transverse energy jet and large missing transverse energy in 2.4 fb{sup -1} of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron p{bar p} collider. Production of such particles (quirks) is expected in scenarios with extra QCD-like SU(N) sectors, and this study is the first dedicated search for such signatures. We find no evidence of a signal and set a lower mass limit of 107 GeV for the mass of a charged quirk with strong dynamics scale {Lambda} in the range from 10 keV to 1 MeV.

  18. Beta Function Measurement in the Tevatron Using Quadrupole Gradient Modulation

    CERN Document Server

    Jansson, Andreas; Volk, James T

    2005-01-01

    Early in Run2, there was an effort to compare the different emittance measurements in the Tevatron (flying wires and synchtotron light) and understand the origin of the observed differences. To measure the beta function at a few key locations near the instruments, air-core quadrupoles were installed. By modulating the gradient of these magents and measuring the effect on the tune, the lattice parameters can be extracted. Initially, the results seem to disagree with with other methods. At the time, the lattice was strongly coupled due to a skew component in the main dipoles, caused by sagging of the cryostat. After a large fraction of the superconducting magnets were shimmed to remove a strong skew quadrupole component, the results now agree with expectations, confirming that the beta function is not the major error source of discrepancy in the emittance measurement.

  19. Measurements of the Top Quark at the Tevatron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Cerrito, Lucio

    2007-01-01

    The authors present recent preliminary measurements of the top-antitop pair production cross section and determinations of the top quark pole mass, performed using the data collected by the CDF and D0 Collaborations at the Tevatron Collider. In the lepton plus jets final state, with semileptonic B decay, the pair production cross section has now been measured at CDF using {approx} 760 pb{sup -1} of proton-antiproton collisions at a center-of-mass energy of {radical}s = 1.96 TeV. A measurement of the production cross section has also been made with {approx} 1 fb{sup -1} of data in the all-jets final state by the CDF Collaboration. The mass of the top quark has now been measured using {approx} 1 fb{sup -1} of collision data using all decay channels of the top quark pair, yielding the most precise measurements of the top mass to date.

  20. W/Z + Jets production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Yu, J. [Univ. of Rochester, NY (United States)

    1995-07-01

    Both the D0 and CDF experiments at Fermilab Tevatron collider at {radical}s = 1.8 TeV have accumulated over 50pb{sup -1} of data. Each experiment collected more than 50,000 W {yields} l +v and 5000 Z {yields} l + {bar l} candidates for each lepton species (e and {mu}). Using this large data sample of W and Z candidates, the two experiments are actively testing perturbative QCD predictions. Among the studies that are in progress, preliminary results of W/Z+jets characteristics, multiplicity distributions of associated jets, and a study on the determination of the strong coupling constant using the ratio of the W+1 jet to W + 0 jet cross sections are presented.

  1. Search for new fermions ("quirks") at the Fermilab Tevatron collider.

    Science.gov (United States)

    Abazov, V M; Abbott, B; Abolins, M; Acharya, B S; Adams, M; Adams, T; Alexeev, G D; Alkhazov, G; Alton, A; Alverson, G; Alves, G A; Ancu, L S; Aoki, M; Arnoud, Y; Arov, M; Askew, A; Asman, B; Atramentov, O; Avila, C; Backusmayes, J; Badaud, F; Bagby, L; Baldin, B; Bandurin, D V; Banerjee, S; Barberis, E; Baringer, P; Barreto, J; Bartlett, J F; Bassler, U; Beale, S; Bean, A; Begalli, M; Begel, M; Belanger-Champagne, C; Bellantoni, L; Benitez, J A; Beri, S B; Bernardi, G; Bernhard, R; Bertram, I; Besançon, M; Beuselinck, R; Bezzubov, V A; Bhat, P C; Bhatnagar, V; Blazey, G; Blessing, S; Bloom, K; Boehnlein, A; Boline, D; Bolton, T A; Boos, E E; Borissov, G; Bose, T; Brandt, A; Brandt, O; Brock, R; Brooijmans, G; Bross, A; Brown, D; Brown, J; Bu, X B; Buchholz, D; Buehler, M; Buescher, V; Bunichev, V; Burdin, S; Burnett, T H; Buszello, C P; Calpas, B; Calvet, S; Camacho-Pérez, E; Carrasco-Lizarraga, M A; Carrera, E; Casey, B C K; Castilla-Valdez, H; Chakrabarti, S; Chakraborty, D; Chan, K M; Chandra, A; Chen, G; Chevalier-Théry, S; Cho, D K; Cho, S W; Choi, S; Choudhary, B; Christoudias, T; Cihangir, S; Claes, D; Clutter, J; Cooke, M; Cooper, W E; Corcoran, M; Couderc, F; Cousinou, M-C; Croc, A; Cutts, D; Cwiok, M; Das, A; Davies, G; De, K; de Jong, S J; De La Cruz-Burelo, E; Déliot, F; Demarteau, M; Demina, R; Denisov, D; Denisov, S P; Desai, S; Devaughan, K; Diehl, H T; Diesburg, M; Dominguez, A; Dorland, T; Dubey, A; Dudko, L V; Duggan, D; Duperrin, A; Dutt, S; Dyshkant, A; Eads, M; Edmunds, D; Ellison, J; Elvira, V D; Enari, Y; Eno, S; Evans, H; Evans, J A; Evdokimov, A; Evdokimov, V N; Facini, G; Ferapontov, A V; Ferbel, T; Fiedler, F; Filthaut, F; Fisher, W; Fisk, H E; Fortner, M; Fox, H; Fuess, S; Gadfort, T; Garcia-Bellido, A; Gavrilov, V; Gay, P; Geist, W; Geng, W; Gerbaudo, D; Gerber, C E; Gershtein, Y; Ginther, G; Golovanov, G; Goussiou, A; Grannis, P D; Greder, S; Greenlee, H; Greenwood, Z D; Gregores, E M; Grenier, G; Gris, Ph; Grivaz, J-F; Grohsjean, A; Grünendahl, S; Grünewald, M W; Guo, F; Guo, J; Gutierrez, G; Gutierrez, P; Haas, A; Hagopian, S; Haley, J; Han, L; Harder, K; Harel, A; Hauptman, J M; Hays, J; Hebbeker, T; Hedin, D; Hegab, H; Heinson, A P; Heintz, U; Hensel, C; Heredia-De La Cruz, I; Herner, K; Hesketh, G; Hildreth, M D; Hirosky, R; Hoang, T; Hobbs, J D; Hoeneisen, B; Hohlfeld, M; Hossain, S; Hubacek, Z; Huske, N; Hynek, V; Iashvili, I; Illingworth, R; Ito, A S; Jabeen, S; Jaffré, M; Jain, S; Jamin, D; Jesik, R; Johns, K; Johnson, M; Johnston, D; Jonckheere, A; Jonsson, P; Joshi, J; Juste, A; Kaadze, K; Kajfasz, E; Karmanov, D; Kasper, P A; Katsanos, I; Kehoe, R; Kermiche, S; Khalatyan, N; Khanov, A; Kharchilava, A; Kharzheev, Y N; Khatidze, D; Kirby, M H; Kohli, J M; Kozelov, A V; Kraus, J; Kumar, A; Kupco, A; Kurča, T; Kuzmin, V A; Kvita, J; Lammers, S; Landsberg, G; Lebrun, P; Lee, H S; Lee, S W; Lee, W M; Lellouch, J; Li, L; Li, Q Z; Lietti, S M; Lim, J K; Lincoln, D; Linnemann, J; Lipaev, V V; Lipton, R; Liu, Y; Liu, Z; Lobodenko, A; Lokajicek, M; Love, P; Lubatti, H J; Luna-Garcia, R; Luty, M A; Lyon, A L; Maciel, A K A; Mackin, D; Madar, R; Magaña-Villalba, R; Malik, S; Malyshev, V L; Maravin, Y; Martínez-Ortega, J; McCarthy, R; McGivern, C L; Meijer, M M; Melnitchouk, A; Menezes, D; Mercadante, P G; Merkin, M; Meyer, A; Meyer, J; Mondal, N K; Muanza, G S; Mulhearn, M; Nagy, E; Naimuddin, M; Narain, M; Nayyar, R; Neal, H A; Negret, J P; Neustroev, P; Nilsen, H; Novaes, S F; Nunnemann, T; Obrant, G; Onoprienko, D; Orduna, J; Osman, N; Osta, J; Otero Y Garzón, G J; Owen, M; Padilla, M; Pangilinan, M; Parashar, N; Parihar, V; Park, S K; Parsons, J; Partridge, R; Parua, N; Patwa, A; Penning, B; Perfilov, M; Peters, K; Peters, Y; Petrillo, G; Pétroff, P; Piegaia, R; Piper, J; Pleier, M-A; Podesta-Lerma, P L M; Podstavkov, V M; Pol, M-E; Polozov, P; Popov, A V; Prewitt, M; Price, D; Protopopescu, S; Qian, J; Quadt, A; Quinn, B; Rangel, M S; Ranjan, K; Ratoff, P N; Razumov, I; Renkel, P; Rich, P; Rijssenbeek, M; Ripp-Baudot, I; Rizatdinova, F; Rominsky, M; Royon, C; Rubinov, P; Ruchti, R; Safronov, G; Sajot, G; Sánchez-Hernández, A; Sanders, M P; Sanghi, B; Santos, A S; Savage, G; Sawyer, L; Scanlon, T; Schamberger, R D; Scheglov, Y; Schellman, H; Schliephake, T; Schlobohm, S; Schwanenberger, C; Schwienhorst, R; Sekaric, J; Severini, H; Shabalina, E; Shary, V; Shchukin, A A; Shivpuri, R K; Simak, V; Sirotenko, V; Skubic, P; Slattery, P; Smirnov, D; Smith, K J; Snow, G R; Snow, J; Snyder, S; Söldner-Rembold, S; Sonnenschein, L; Sopczak, A; Sosebee, M; Soustruznik, K; Spurlock, B; Stark, J; Stolin, V; Stoyanova, D A; Strauss, E; Strauss, M; Strom, D; Stutte, L; Svoisky, P; Takahashi, M; Tanasijczuk, A; Taylor, W; Titov, M; Tokmenin, V V; Tsybychev, D; Tuchming, B; Tully, C; Tuts, P M; Uvarov, L; Uvarov, S; Uzunyan, S; Van Kooten, R; van Leeuwen, W M; Varelas, N; Varnes, E W; Vasilyev, I A; Verdier, P; Vertogradov, L S; Verzocchi, M; Vesterinen, M; Vilanova, D; Vint, P; Vokac, P; Wahl, H D; Wang, M H L S; Warchol, J; Watts, G; Wayne, M; Weber, M; Wetstein, M; White, A; Wicke, D; Williams, M R J; Wilson, G W; Wimpenny, S J; Wobisch, M; Wood, D R; Wyatt, T R; Xie, Y; Xu, C; Yacoob, S; Yamada, R; Yang, W-C; Yasuda, T; Yatsunenko, Y A; Ye, Z; Yin, H; Yip, K; Yoo, H D; Youn, S W; Yu, J; Zelitch, S; Zhao, T; Zhou, B; Zhu, J; Zielinski, M; Zieminska, D; Zivkovic, L

    2010-11-19

    We report results of a search for particles with anomalously high ionization in events with a high transverse energy jet and large missing transverse energy in 2.4 fb⁻¹ of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron pp collider. Production of such particles (quirks) is expected in scenarios with extra QCD-like SU(N) sectors, and this study is the first dedicated search for such signatures. We find no evidence of a signal and set a lower mass limit of 107, 119, and 133 GeV for the mass of a charged quirk with strong dynamics scale Λ in the range from 10 keV to 1 MeV and N=2, 3, and 5, respectively.

  2. Correlations in bottom quark pair production at the Fermilab Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Galyardt, Jason Edward [Carnegie Mellon Univ., Pittsburgh, PA (United States)

    2009-01-01

    I present an analysis of b$\\bar{b}$ pair production correlations, using dimuon-triggered data collected with the Collider Detector at Fermilab (CDF) in p$\\bar{p}$ collisions at √s = 1.96 TeV during Run II of the TeVatron. The leading order (LO) and next-to-leading order (NLO) b quark production processes are discriminated by the angular and momentum correlations between the b{bar b} pair. Track-level jets containing a muon are classified by b quark content and used to estimate the momentum vector of the progenitor b quark. The theoretical distributions given by the MC@NLO event generator are tested against the data.

  3. Le Procès de Tôkyô, l’empereur et la question du Yasukuni*

    OpenAIRE

    Takahashi, Tetsuya

    2010-01-01

    Au Japon, toute une partie de la classe politique conservatrice persiste à refuser les conclusions du procès de Tôkyô, considérant celui-ci comme une justice « orchestrée par les vainqueurs ». Ce faisant, les partisans de cette thèse se trouvent dans une contradiction puisque l’empereur Hirohito lui-même, qui avait exprimé sa gratitude auprès des forces d’occupation américaines pour l’avoir épargné, en avait de facto admis les conclusions. Ce paradoxe pour le camp conservateur est aggravé par...

  4. Letter of Intent for a Tevatron Collider Beauty Factory

    Energy Technology Data Exchange (ETDEWEB)

    Volk, J.T.; Yager, P.M.; Edelstein, R.; /Carnegie Mellon U.; Christian, D.; /Fermilab; Lundberg, B.; Reay, N.W.; Reibel, K.; Sidwell, R.A.; Stanton, N.; /Ohio State U.; Kalbfleisch, G.R.; Skubic, P.; /Oklahoma U.

    1987-01-01

    A hadron collider beauty production experiment which will increase our knowledge of mixing, rare decay modes and even of CP violation could be performed using a new type of detector at the upgraded Fermilab Tevatron. In order to progress from the hundreds of thousands of B{bar B} events which can be tagged per year at a luminosity of several times 10{sup 29}/cm{sup 2}-sec to an ultimate yield of tens of millions at a luminosity of several times 10{sup 31}/cm{sup 2}-sec, they also must embark on a learning curve which will take many years and will require development both of hardware and software before achieving a final system. A new high-luminosity intersection region would have to be included as part of the presently-planned Tevatron Collider upgrade. Designing and constructing an initial system will take four years. Thus, in the light of the positive decision on the SSC, a start must be made soon if Fermilab is ever to play a strong role in this exciting area of physics. Designing even the initial system will require several man-years of effort by a dedicated group of people, together with concurrent work in prototyping and testing. They therefore ask that the Physics Advisory Committee give us their opinion of the priority such a project should be given at Fermilab, within the context that eventually it will require a devoted interaction region which accesses the full achieved luminosity of the machine. Initially, they discuss physics accessible as the B{bar B} yield increases. Subsequently, they outline a detector which can be staged, increasing its power (and cost) as we progress along our learning curve. Finally, costs and time schedules are estimated for the initial version of this detector and possible locations are discussed.

  5. The Origination and Diagnostics of Uncaptured Beam in the Tevatron and Its Control by Electron Lenses

    CERN Document Server

    Zhang, Xiao-Long; Kamerdzhiev, Vsevolod; Lebedev, Valery; Shiltsev, Vladimir; Thurman-Keup, Randy; Tollestrup, Alvin V

    2008-01-01

    In the Collider Run II, the Tevatron operates with 36 high intensity bunches of 980 GeV protons and antiprotons. Particles not captured by the Tevatron RF system pose a threat to quench the superconducting magnet during acceleration or at beam abort. We describe the main mechanisms for the origination of this uncaptured beam, and present measurements of its main parameters by means of a newly developed diagnostics system. The Tevatron Electron Lens is effectively used in the Collider Run II operation to remove uncaptured beam and keep its intensity in the abort gaps at a safe level.

  6. Generation and diagnostics of uncaptured beam in the Fermilab Tevatron and its control by electron lenses

    Science.gov (United States)

    Zhang, Xiao-Long; Bishofberger, Kip; Kamerdzhiev, Vsevolod; Lebedev, Valery; Shiltsev, Vladimir; Thurman-Keup, Randy; Tollestrup, Alvin

    2008-05-01

    In the collider run II, the Tevatron operates with 36 high intensity bunches of 980 GeV protons and antiprotons. Particles not captured by the Tevatron rf system pose a threat since they can quench the superconducting magnets during acceleration or at beam abort. We describe the main mechanisms for the origination of this uncaptured beam, and present measurements of its main parameters by means of a newly developed diagnostics system. The Tevatron electron lens is effectively used in the collider run II operation to remove uncaptured beam and keep its intensity in the abort gaps at a safe level.

  7. QCD analysis of $W$- and $Z$-boson production at Tevatron

    CERN Document Server

    Camarda, S; Cooper-Sarkar, A M; Diaconu, C; Glazov, A; Guffanti, A; Jung, A; Kolesnikov, V; Lohwasser, K; Myronenko, V; Olness, F; Pirumov, H; Placakyte, R; Radescu, V; Sapronov, A; Slominski, W; Starovoitov, P

    2015-01-01

    Recent measurements of the $W$-boson charge asymmetry and of the $Z$-boson production cross sections, performed at the Tevatron collider in Run II by the D0 and CDF collaborations, are studied to assess their impact on the proton parton distribution functions (PDFs), using the \\HERAFitter framework. The Tevatron measurements, together with deep-inelastic scattering data from HERA, are included in a QCD analysis performed at next-to-leading order, and compared to the predictions obtained using other PDF sets from different groups. Good agreement between measurements and theoretical predictions is observed. The Tevatron data provide significant constraints on the $d$-valence quark distribution.

  8. Detecting a light Higgs boson at the Fermilab Tevatron through enhanced decays to photon pairs

    CERN Document Server

    Mrenna, S; Mrenna, Stephen; Wells, James

    2001-01-01

    We analyze the prospects of the Tevatron for finding a Higgs boson in the two photon decay mode. We conclude that the Standard Model (SM) Higgs boson will likely not be discovered in this mode. However, we motivate several theories beyond the SM, including the MSSM, that predict a Higgs boson with enhanced branching fractions into photons, and calculate the luminosity needed to discover a general Higgs boson at the Tevatron by a two-photon invariant mass peak at large transverse momentum. We find that a high luminosity Tevatron will play a significant role in discovering or constraining these theories.

  9. QCD analysis of W- and Z-boson production at Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Camarda, S.; Glazov, A.; Myronenko, V.; Pirumov, H.; Placakyte, R.; Starovoitov, P. [Deutsches Elektronen-Synchrotron (DESY), Hamburg (Germany); Belov, P. [Deutsches Elektronen-Synchrotron (DESY), Hamburg (Germany); St. Petersburg State University, Department of Physics, St. Petersburg (Russian Federation); Cooper-Sarkar, A.M. [University of Oxford, Department of Physics, Oxford (United Kingdom); Diaconu, C. [Univ. Mediterranee, CPPM, IN2P3-CNRS, Marseille (France); Guffanti, A. [University of Copenhagen, Niels Bohr International Academy and Discovery Center, Niels Bohr Institute, Copenhagen (Denmark); Jung, A. [Fermilab, Batavia, IL (United States); Kolesnikov, V.; Sapronov, A. [Joint Institute for Nuclear Research (JINR), Dubna, Moscow Region (Russian Federation); Lohwasser, K. [Deutsches Elektronen-Synchrotron (DESY), Zeuthen (Germany); Olness, F. [Southern Methodist University, Dallas, TX (United States); Radescu, V. [Universitaet Heidelberg, Physikalisches Institut, Heidelberg (Germany); Slominski, W. [Jagiellonian University, M. Smoluchowski Institute of Physics, Cracow (Poland); Sutton, M. [University of Sussex, Department of Physics and Astronomy, Brighton (United Kingdom); Collaboration: HERAFitter developers' team

    2015-09-15

    Recent measurements of the W-boson charge asymmetry and of the Z-boson production cross sections, performed at the Tevatron collider in Run II by the D0 and CDF collaborations, are studied using the HERAFitter framework to assess their impact on the proton parton distribution functions (PDFs). The Tevatron measurements, together with deep-inelastic scattering data from HERA, are included in a QCD analysis performed at next-to-leading order, and compared to the predictions obtained using other PDF sets from different groups. Good agreement between measurements and theoretical predictions is observed. The Tevatron data provide significant constraints on the d-valence quark distribution. (orig.)

  10. QCD analysis of W- and Z-boson production at Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Camarda, S. [Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, 22607, Hamburg (Germany); Belov, P. [Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, 22607, Hamburg (Germany); Department of Physics, St. Petersburg State University, Ulyanovskaya 1, 198504, St. Petersburg (Russian Federation); Cooper-Sarkar, A. M. [Department of Physics, University of Oxford, Oxford (United Kingdom); Diaconu, C. [CPPM, IN2P3-CNRS, Univ. Mediterranee, Marseille (France); Glazov, A. [Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, 22607, Hamburg (Germany); Guffanti, A. [Niels Bohr International Academy and Discovery Center, Niels Bohr Institute, University of Copenhagen, Blegdamsvej 17, 2100, Copenhagen (Denmark); Jung, A. [FERMILAB, 60510, Batavia, IL (United States); Kolesnikov, V. [Joint Institute for Nuclear Research (JINR), Joliot-Curie 6, 141980, Dubna, Moscow Region (Russian Federation); Lohwasser, K. [Deutsches Elektronen-Synchrotron (DESY), Platanenallee 6, 15738, Zeuthen (Germany); Myronenko, V. [Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, 22607, Hamburg (Germany); Olness, F. [Southern Methodist University, Dallas, TX (United States); Pirumov, H.; Plačakytė, R. [Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, 22607, Hamburg (Germany); Radescu, V. [Physikalisches Institut, Universität Heidelberg, Heidelberg (Germany); Sapronov, A. [Joint Institute for Nuclear Research (JINR), Joliot-Curie 6, 141980, Dubna, Moscow Region (Russian Federation); Slominski, W. [M. Smoluchowski Institute of Physics, Jagiellonian University, Cracow (Poland); Starovoitov, P. [Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, 22607, Hamburg (Germany); Sutton, M. [Department of Physics and Astronomy, University of Sussex, Sussex House, BN1 9RH, Brighton (United Kingdom)

    2015-09-28

    Recent measurements of the W-boson charge asymmetry and of the Z-boson production cross sections, performed at the Tevatron collider in Run II by the D0 and CDF collaborations, are studied using the HERAFitter framework to assess their impact on the proton parton distribution functions (PDFs). The Tevatron measurements, together with deep-inelastic scattering data from HERA, are included in a QCD analysis performed at next-to-leading order, and compared to the predictions obtained using other PDF sets from different groups. Good agreement between measurements and theoretical predictions is observed. The Tevatron data provide significant constraints on the d-valence quark distribution.

  11. La gestion de la relation client dans la banque: Cas du marché marocain

    Directory of Open Access Journals (Sweden)

    EL KORAICHI Mustapha

    2014-03-01

    Full Text Available Face aux évolutions du secteur bancaire (concurrence accrue, crise de confiance l’adoption d’un système de gestion de la relation client représente un enjeu important pour les banques. Il contribue à l’optimisation de la gestion du portefeuille client, plus précisément ce système permet d’acquérir de nouveaux clients et d’augmenter la rentabilité des clients existants. Cet article a pour objectif de répondre à la problématique suivante: le système de gestion de la relation client permet-il aux banques d’atteindre les objectifs attendus? L’étude que nous avons réalisée auprès de 47 banques commerciales marocaines montre que malgré le potentiel anticipé, les bénéfices escomptés d’un tel système restent limités. En effet, l’utilisation de ce système reste à son état embryonnaire, il se centre principalement sur la collecte des informations clients au niveau des agences tandis que l’analyse et l’exploitation de ces informations se fait au niveau du siège de la banque. De même, les opérations basiques de la banque occupent une grande part du temps de travail des agents de la banque au dépend des services bancaires à valeur ajoutée. D’un autre côté, une grande part des banques adoptant ce système ne mesurent pas le coût de la relation avec leurs clients.

  12. Study of dimuon spectrometer tracking chambers of the ALICE experiment at LHC; Etude des chambres de trajectoire du spectrometre dimuons de l'experience ALICE aupres du LHC

    Energy Technology Data Exchange (ETDEWEB)

    Kharmandarian, Liliane [Institut de Physique Nucleaire, CNRS - IN2P3, Universite Paris - Sud, 91406 Orsay Cedex (France)

    1999-12-16

    The ALICE (A Large Ion Collider Experiment) experiment will study ultrarelativistic heavy ion collisions at the Large Hadron Collider (LHC) in CERN as of 2005. An extensive R and D programme has been carried out on the dimuon spectrometer tracking chambers at the Nuclear Physics Institute in Orsay. Three multiwire proportional chamber prototypes with segmented cathodes, including a full-scale 1 m{sup 2} version, were constructed. In this thesis, the experimental tests are presented along with the simulations used to understand and optimize the detectors' performances. The prototypes were tested several times at the PS and SPS accelerators. The aims were to validate the choices made in terms of mechanical construction, geometrical parameters, gas mixture and read-out electronics. Analysis of the large amount of data collected has shown that the performances of this type of detector fulfill the required specifications. The results concerning the detectors' characteristics, spatial resolution efficiency, gain and homogeneity are given. Spatial resolutions of less than thirty microns were obtained. In parallel with the in-beam tests, several simulations have been developed in order to gain a better understanding of the detectors' response. They allowed, in particular, to define the segmentation of the cathode plane, to study the position reconstruction algorithm and to establish the future electronics specifications. (author)

  13. Recherche du boson de Higgs chargé dans le canal H+ -> tb et étiquetage des jets b avec l'expérience ATLAS auprès du LHC.

    CERN Document Server

    Zaidan, R

    The only particle of the Standard Model that has not yet been discovered is the Higgs boson, which explains the origin of the masses of elementary particles. In the Minimal Supersymmetric extention to the Standard Model (MSSM), the Higgs sector consists of five bosons, two of which are charged. The search for a charged Higgs boson in the gg ¯tbH+(H+ ! t¯b) channel, is the main topic of this analysis. We present an analysis that uses a likelihood function to resolve combinatorics while reconstructing the charged Higgs boson, and the b-tagging to suppress the t¯t+jets background. We also present the difficulties due to the combinatoric background reducing the discovery potential of this channel. The presence of 4 b quarks in the final state that we are looking at, makes the b-tagging an important tool for the analysis. Therefore, a part of this work is dedicated to the study of b-tagging. We present in the context of the preperation for the first data, several studies dedicated to the optimisation and the un...

  14. Prospects for diffractive physics with the CDF forward detectors at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    M. Gallinaro [and others

    2002-07-09

    The Forward Detector upgrade project at CDF is designed to enhance the capabilities for studies of diffractive physics at the Tevatron during Run II. Studies of hard diffraction and very forward physics are some of the topics that can be addressed in the next few years at the Tevatron. The program for diffractive physics, including the detectors and their commissioning, is discussed here. All the detectors have been installed and are presently collecting data.

  15. Present status and future prospects for a Higgs boson discovery at the Tevatron and LHC

    CERN Document Server

    Haber, Howard E

    2010-01-01

    Discovering the Higgs boson is one of the primary goals of both the Tevatron and the Large Hadron Collider (LHC). The present status of the Higgs search is reviewed and future prospects for discovery at the Tevatron and LHC are considered. This talk focuses primarily on the Higgs boson of the Standard Model and its minimal supersymmetric extension. Theoretical expectations for the Higgs boson and its phenomenological consequences are reviewed.

  16. Diffractive Higgs boson production at the Fermilab Tevatron and the CERN Large Hadron Collider.

    Science.gov (United States)

    Enberg, R; Ingelman, G; Kissavos, A; Tîmneanu, N

    2002-08-19

    Improved possibilities to find the Higgs boson in diffractive events, having less hadronic activity, depend on whether the cross section is large enough. Based on the soft color interaction models that successfully describe diffractive hard scattering at DESY HERA and the Fermilab Tevatron, we find that only a few diffractive Higgs events may be produced at the Tevatron, but we predict a substantial rate at the CERN Large Hadron Collider.

  17. Radiation measurements in the reactors G 2 and G 3; Mesures de rayonnement aupres des piles G 2 - G 3

    Energy Technology Data Exchange (ETDEWEB)

    Chassany, J.Ph.; Estournel, R. [Commissariat a l' Energie Atomique, Centre de Production de Plutonium, Marcoule (France). Centre d' Etudes Nucleaires

    1964-07-01

    The results are given of numerous radiation measurements: - for the various working sites - for the various zones (circuit room,etc) - during the discharging operations - far various active materials (CO{sub 2}, plugs etc). They show that in general the protection has been suitably designed and that the majority of radio-protection problems are due to the elements activated in the pile and transported outside the vessel. (authors) [French] Les resultats de nombreuses mesures d'irradiation sont donnes - pour les differents lieux de travail - pour diverses zones (salle de tuyauteries, etc.) - pendant les operations de dechargement - pour differents materiaux actives (CO{sub 2}, bouchons, etc.) Ils montrent que les protections ont ete en general correctement dimensionnees et que la majorite des problemes de radioprotection est constituee par les elements actives dans la pile, transportes a l'exterieur du caisson. (auteurs)

  18. The Charlie Hebdo Terror Attack in Paris: Follow-up of French Citizens’ Terrorist Threat Perception and Its Aftermath [L’attaque Terroriste de Charlie Hebdo à Paris : Evolution temporelle de la Perception de la Menace Terroriste et de ses Conséquences auprès des Citoyens Français

    Directory of Open Access Journals (Sweden)

    Petra Pelletier

    2016-08-01

    Full Text Available Terrorism is one of the most frightful large-scale societal threats nowadays. The January 7, 2015 Charlie Hebdo terrorist attack in Paris shattered French’s sense of security. The present research investigates French citizen’s ('N' = 160 terrorist threat perception (personal vs. collective, behavioral changes, social sharing of emotions and perceived socioemotional climate using the social stage model of collective coping with disasters (Pennebaker & Harber, 1993. This study was conducted by a questionnaire at three points of time (i.e., one week, one month and two month following the attack. The results suggest that terrorist threat perception has not decreased across time at the personal level nor at the collective level. However, the extent of social sharing of emotions and the positive socioemotional climate decreased from the initial emergency stage to the subsequent adaptation stage. Such findings point to the importance of taking temporality into account to provide better understanding of lay people’s responses to terrorism. Résumé Le terrorisme est l’une des menaces sociétales à grande échelle les plus effroyables de nos jours. L’attaque terroriste de Charlie Hebdo du 7 janvier 2015 à Paris a ébranlé le sentiment de sécurité des Français. La présente recherche examine la perception de la menace terroriste (personnelle vs. collective, les changements comportementaux, le partage social des émotions et le climat socio-émotionnel perçu auprès des citoyens français (N = 160 en se basant sur le modèle des étapes sociales de coping collectif avec les catastrophes (Pennebaker & Harber, 1993. Cette étude a été conduite par questionnaire à trois points temporels (c.-à-d., une semaine, un mois et deux mois après l’attaque. Les résultats suggèrent que la perception de la menace terroriste n’a pas diminué à travers le temps, ni au niveau personnel, ni au niveau collectif. Toutefois, l’ampleur du partage

  19. Des limbes du symbolique a l’acte d’auteurisation ou de la fonction sinthomatique de l’usage des tests en psychologie clinique

    Directory of Open Access Journals (Sweden)

    Laetitia Sublime

    Full Text Available Cet article a pour origine une pratique de psychologue clinicienne auprès de patients séropositifs que j’ai choisi de situer hors d’une sémiologie classique en postulant une “pathologie des limbes du symbolique”. Je montrerai comment l’usage des tests ne saurait se déprendre des exigences d’une clinique de la subjectivité en restituant à ces outils – considérés comme autant de “renversements dialectiques” et de scansions du discours – leur place légitime dans une clinique de la parole et du langage. L’offre de supports narratifs prothétiques pourrait encourager l’advenue d’une fonction sinthomatique, acte d’auteurisation par la relance de l’élaboration symbolique autour du trauma, appel au travail de la mémoire et à la reconstruction d’une histoire demeurée jusque là sans destinataire, dans les limbes.

  20. La profanation du montage

    OpenAIRE

    Hildebrandt, Toni

    2017-01-01

    Cet article examine les liens entre, pour l’aspect technique, le plan séquence et le montage, et, pour l’aspect philosophico-historique, la vie quotidienne et la politique mondiale, du point de vue d’une profanation capable de désamorcer la puissance et avec une attention particulière portée à l’unique film expérimental de Pasolini : La sequenza del fiore di (1968). Ce court métrage n’a pas seulement un statut spécial dans la filmographie de Pasolini, il marque aussi un tournant du tragique v...

  1. W mass and Triple Gauge Couplings at Tevatron

    Directory of Open Access Journals (Sweden)

    Pétroff Pierre

    2013-05-01

    Full Text Available The W mass is a crucial parameter in the Standard Model (SM of particle physics, providing constraints on the mass of the Higgs boson as well as on new physics models via quantum loop corrections. On the other hand, any deviation of the triple gauge boson couplings (TGC from their values predicted by the SM would be also an indication for new physics. We present recent measurements on W boson mass and searches for anomalous TGC (aTGC in Wγ, Zγ, WW, WZ and ZZ at Fermilab Tevatron both by CDF and DØ Collaborations. The CDF Collaboration has measured the W boson mass using data corresponding to 2.2 fb−1 of integrated luminosity. The measurement, performed using electron and muon decays of W boson, yields a mass of MW = 80387 ± 19 MeV. The DØ Collaboration has measured MW = 80367 ± 26 MeV with data corresponding to 4.3 fb−1 of integrated luminosity in the channel W → ev. The combination with an earlier DØ result, using independant data sample at 1 fb−1 of integrated luminosity, yields MW = 80375 ± 23 MeV. The limits on anomalous TGCs parameters are consistent with the SM expectations.

  2. Heavy Flavour Production at Tevatron and Parton Shower Effects

    CERN Document Server

    Jung, H; Lipatov, A V; Zotov, N P

    2010-01-01

    We present hadron-level predictions from the Monte Carlo generator Cascade and numerical calculations of charm and beauty production at the Fermilab Tevatron within the framework of the $k_T$-factorization QCD approach. Our consideration is based on the CCFM-evolved unintegrated gluon densities in a proton. The performed analysis covers the total and differential cross sections of open charm and beauty quarks, $B$ and $D$ mesons (or rather muons from their semileptonic decays) and the total and differential cross sections of $b \\bar b$ di-jet hadroproduction. We study the theoretical uncertainties of our calculations and investigate the effects coming from parton showers in initial and final states. Our predictions are compared with the recent experimental data taken by the D0 and CDF collaborations. Special attention is put on the specific angular correlations between the final-state particles. We demonstrate that the final state parton shower plays a crucial role in the description of such observables. The ...

  3. Heavy flavour production at Tevatron and parton shower effects

    Energy Technology Data Exchange (ETDEWEB)

    Jung, H. [Deutsches Elektronen-Synchrotron (DESY), Hamburg (Germany); Antwerp Univ. (Belgium); Kraemer, M. [Deutsches Elektronen-Synchrotron (DESY), Hamburg (Germany); Lipatov, A.V.; Zotov, N.P. [M.V. Lomonosov Moscow State Univ. (Russian Federation). D.V. Skobeltsyn Inst. of Nuclear Physics

    2010-09-15

    We present hadron-level predictions from the Monte Carlo generator Cascade and numerical calculations of charm and beauty production at the Fermilab Tevatron within the framework of the k{sub T}-factorization QCD approach. Our consideration is based on the CCFMevolved unintegrated gluon densities in a proton. The performed analysis covers the total and differential cross sections of open charm and beauty quarks, B and D mesons (or rather muons from their semileptonic decays) and the total and differential cross sections of b anti b di-jet hadroproduction. We study the theoretical uncertainties of our calculations and investigate the effects coming from parton showers in initial and final states. Our predictions are compared with the recent experimental data taken by the D0 and CDF collaborations. Special attention is put on the specific angular correlations between the final-state particles. We demonstrate that the final state parton shower plays a crucial role in the description of such observables. The decorrelated part of angular separations can be fully described, if the process gg{sup *} {yields} gg is included. (orig.)

  4. Progress in Antiproton Production at the Fermilab Tevatron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Pasquinelli, Ralph J.; Drendel, Brian; Gollwitzer, Keith; Johnson, Stan; Lebedev, Valeri; Leveling, Anthony; Morgan, James; Nagaslaev, Vladimir; Peterson, Dave; Sondgeroth, Alan; Werkema, Steve; /Fermilab

    2009-04-01

    Fermilab Collider Run II has been ongoing since 2001. During this time peak luminosities in the Tevatron have increased from approximately 10 x 10{sup 30} cm{sup -2}sec{sup -1} to 300 x 10{sup 30} cm{sup 02}sec{sup -1}. A major contributing factor in this remarkable performance is a greatly improved antiproton production capability. Since the beginning of Run II, the average antiproton accumulation rate has increased from 2 x 10{sup 10}{anti p}/hr to about 24 x 10{sup 10}{anti p}/hr. Peak antiproton stacking rates presently exceed 28 x 10{sup 10}{anti p}/hr. The antiproton stacking rate has nearly doubled since 2005. It is this recent progress that is the focus of this paper. The process of transferring antiprotons to the Recycler Ring for subsequent transfer to the collider has been significantly restructured and streamlined, yielding additional cycle time for antiproton production. Improvements to the target station have greatly increased the antiproton yield from the production target. The performance of the Antiproton Source stochastic cooling systems has been enhanced by upgrades to the cooling electronics, accelerator lattice optimization, and improved operating procedures. In this paper, we will briefly report on each of these modifications.

  5. Probing neutrino mass with displaced vertices at the Tevatron

    CERN Document Server

    De Campos, F; Magro, M B; Porod, Werner; Restrepo, D; Valle, J W F

    2005-01-01

    Supersymmetric extensions of the standard model exhibiting bilinear R-parity violation can generate naturally the observed neutrino mass spectrum as well mixings. One interesting feature of these scenarios is that the lightest supersymmetric particle (LSP) is unstable, with several of its decay properties predicted in terms of neutrino mixing angles. A smoking gun of this model in colliders is the presence of displaced vertices due to LSP decays in large parts of the parameter space. In this work we focus on the simplest model of this type that comes from minimal supergravity with universal R-parity conserving soft breaking of supersymmetry (RmSUGRA). We evaluate the potentiality of the Fermilab Tevatron to probe the RmSUGRA parameters through the analysis of events possessing two displaced vertices stemming from LSP decays. We show that requiring two displaced vertices in the events leads to a reach in m_{1/2} twice the one in the usual multilepton signals in a large fraction of the parameter space.

  6. Origine du vieux slave

    Directory of Open Access Journals (Sweden)

    Witold Mańczak

    2005-12-01

    Full Text Available Comme, pour prouver l'identité du vieux slave et du vieux bulgare, on invoque uniquement des critères phonétiques, rappelons que l'orientaliste allemand du XVIIe siècle Ludolf affirmait déjà que "die Sprachverwandtschaft offenbart sich nicht im Wörterbuch, sondern in der Grammatik"3. Pendant les 300 dernières années, tellement d'autorites ant approuvé !l’opinion de Ludolf qu'elle est devenue un dogme de la linguistique. Pourtant il nous est venu à l'esprit de le confronter avec des faits et ainsi nous sommes arrivé à la conclusion qu'en réalité, c'est le vocabulaire (et non la phonétique et la flexion qui décide du degre de la parenté des langues4. Voici des arguments à l'appui de cette thèse.

  7. La foret du Banco

    NARCIS (Netherlands)

    Koning, de J.

    1983-01-01

    Deze publicatie over het Nationaal Park 'La Forêt du Banco' nabij Abidjan, Ivoorkust, verschijnt als resultaat van vier jaar veldwerk (1972-1976) in dat land.Het Centre Néerlandais, onderzoeks- en stageverblijf van de Landbouwhogeschool, was basis en de faciliteiten verleend door het Franse ORSTOM-i

  8. Historique du Web

    CERN Multimedia

    TV8 Mont-Blanc

    1995-01-01

    Documentaire court qui retrace l'implication de différentes personalités à la création du Web. Entrevues avec Robert Cailliau, Chris Llewellyn-Smith, David Williams, Tim Berners-Lee, Mike Sendall, Brian Carpenter.

  9. Observation of Central Exclusive Diphoton Production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Brucken, Jens Erik [Univ. of Helsinki (Finland); Helsinki Inst. of Physics (Finland)

    2013-01-01

    We have observed exclusive γγ production in proton-antiproton collisions at the Tevatron at √ s = 1.96 TeV. We use data corresponding to 1.11 ± 0.07 fb-1 integrated luminosity taken by the Run II Collider Detector at Fermilab, with a trigger requiring two electromagnetic showers, each with transverse energy ET > 2 GeV, and vetoing on hits in the forward beam shower counters. We select events with two electromagnetic showers, each with transverse energy ET > 2.5 GeV and pseudorapidity |η| < 1.0, with no other particles detected in -7.4 < η < +7.4. The two showers have similar ET and an azimuthal angle separation Δφ ~ π; we find 34 events with exactly two matching charged particle tracks, agreeing with expectations for the QED process p¯p → p+e+e- + ¯p by two photon exchange; and we find 43 events with no tracks. The latter are candidates for the exclusive process p¯p → p + γγ + ¯p by double pomeron exchange. We use the strip and wire chambers at the longitudinal shower maximum position within the calorimeter to measure a possible exclusive background from IP + IP → π0π0, and conclude that it is consistent with zero and is < 15 events at 95% C.L. The measured cross section is σγγ,excl(|η| < 1, ET (γ) > 2.5 GeV) = 2.48 +0.40 -0.35(stat) +0.40 -0.51(syst) pb and in agreement with the theoretical predictions. This process is closely related to exclusive Higgs boson production pp → p + H + p at the Large Hadron Collider. The observation of the exclusive production of diphotons shows that exclusive Higgs production can happen and could be observed with a proper experimental setup.

  10. 2007 2008 ACADEMIC TRAINING PROGRAMME: Tevatron: The Cinderella Story or The Art Of Collider Commissioning

    CERN Multimedia

    2007-01-01

    LECTURE SERIES 01, 03, 04, 05 October 2007 Main Auditorium, bldg. 500 Tevatron: The Cinderella Story or The Art Of Collider Commissioning V. SHILTSEV / Fermi National Accelerator Laboraty, Batavia IL, USA The Tevatron Collider at Fermilab (Batavia, IL, USA) is the world’s highest energy particle collider at 1.8TeV c.m.e. The machine was a centerpiece of the US and world’s High Energy Physics for many years. Currently, the Tevatron is in the last years of its operation in so-called Run II which started 2001 and is tentatively scheduled to end in 2010. In this lecture series, we’ll try to learn from the exciting story of the Tevatron Collider Run II: the story of long preparations, great expectations, initial difficulties, years of "blood and sweat", continuous upgrades, exceeding its goals, high emotions, tune-up of accelerator organization for "combat fighting". The lectures will cover Introduction to the Tevatron, its history and Run II; "Plumbing"...

  11. Le Procès de Tôkyô, l’empereur et la question du Yasukuni The Tokyo trial, the emperor and the Yasukuni shrine

    OpenAIRE

    Tetsuya Takahashi

    2010-01-01

    Au Japon, toute une partie de la classe politique conservatrice persiste à refuser les conclusions du procès de Tôkyô, considérant celui-ci comme une justice « orchestrée par les vainqueurs ». Ce faisant, les partisans de cette thèse se trouvent dans une contradiction puisque l’empereur Hirohito lui-même, qui avait exprimé sa gratitude auprès des forces d’occupation américaines pour l’avoir épargné, en avait de facto admis les conclusions. Ce paradoxe pour le camp conservateur est aggravé par...

  12. Aux origines du monde

    CERN Multimedia

    2004-01-01

    "C'est l'histoire d'une aventure humaine, scientifique, international qui a vu le jour il y a cinquante ans, aux confins de la Suisse et du département de l'Ain. Le plus grand laboratoire de physique des particules du monde, le Cern, a été fondé en 1954. Les festivités organisées à l occasion de cet anniversaire connaîtront leur point d'orgue le 16 octobre prochain, avec portes-ouvertes, accueil de personallités et inauguration d'un monumnet spécifique, le Globe de l'innovation" (2 pages)

  13. Images du Valais

    Directory of Open Access Journals (Sweden)

    Micheline COSINSCHI

    1995-06-01

    Full Text Available Une étude des revenus fiscaux ventilés par branches économiques permet de clore un ouvrage portant sur ce canton alpin suisse par excellence qu’est le Valais. Pris comme traceurs de l’activité régionale, l’analyse de leurs configurations spatiales permet une évaluation pouvant être considérée comme une mesure de l’efficacité différentielle du système socio-spatial valaisan. L’article décrit certains processus qui ont permis la réalisation du dernier chapitre d’un atlas portant sur le Valais.

  14. CHOEUR DU CERN

    CERN Multimedia

    CHOEUR DU CERN

    2010-01-01

    Les répétitions du chœur du CERN reprendront le mercredi 15 septembre à 20.00 heures à l’amphithéâtre principal – bâtiment 500. Au programme la préparation de notre concert de Noël avec la Missa Brevis, KV115, de Léopold Mozart et de la musique de Noël d’Europe. Les personnes qui aiment chanter, notamment des sopranes et des ténors, sont les bienvenues. Pour tout contact s’adresser à : Baudouin Bleus - (tél.CERN 767 82 44) -(baudouin.bleus@cern.ch) ou Martin Gatehouse ( martin.gatehouse@wanadoo.fr) ou Jean-Paul Diss (jean-pauldiss@wanadoo.fr).  

  15. Perturbative QCD description of jet data from LHC Run-I and Tevatron Run-II

    CERN Document Server

    Carrazza, Stefano

    2014-01-01

    We present a systematic comparison of jet predictions at the LHC and the Tevatron, with accuracy up to next-to-next-to-leading order (NNLO). The exact computation at NNLO is completed for the gluons-only channel, so we compare the exact predictions for this channel with an approximate prediction based on threshold resummation, in order to determine the regions where this approximation is reliable at NNLO. The kinematic regions used in this study are identical to the experimental setup used by recently published jet data from the ATLAS and CMS experiments at the LHC, and CDF and D0 experiments at the Tevatron. We study the effect of choosing different renormalisation and factorisation scales for the NNLO exact prediction and as an exercise assess their impact on a PDF fit including these corrections. Finally we provide numerical values of the NNLO k-factors relevant for the LHC and Tevatron experiments.

  16. Fermilab Tevatron and CERN LEP II probes of minimal and string-motivated supergravity models

    CERN Document Server

    Baer, Howard W; Kao, C; Pois, H

    1995-01-01

    We explore the ability of the Tevatron to probe Minimal Supersymmetry with high energy scale boundary conditions motivated by supersymmetry breaking in the context of supergravity/superstring theory. A number of boundary condition possibilities are considered: dilaton-like string boundary conditions applied at the standard GUT unification scale or alternatively at the string scale; and extreme (``no-scale'') minimal supergravity boundary conditions imposed at the GUT scale or string scale. For numerous specific cases within each scenario the sparticle spectra are computed and then fed into ISAJET 7.07 so that explicit signatures can be examined in detail. We find that, for some of the boundary condition choices, large regions of parameter space can be explored via same-sign dilepton and isolated trilepton signals. For other choices, the mass reach of Tevatron collider experiments is much more limited. We also compare mass reach of Tevatron experiments with the corresponding reach at LEP 200.

  17. Popping out the Higgs boson off vacuum at Tevatron and LHC

    CERN Document Server

    Boonekamp, M; Royon, C

    2003-01-01

    In the prospect of diffractive Higgs production at the LHC collider, we give an extensive study of Higgs boson, dijet, diphoton and dilepton production at hadronic colliders via diffraction at both hadron vertices. Our model, based on non factorizable Pomeron exchange, describes well the observed dijet rate observed at Tevatron Run I. Taking the absolute normalization from data, our predictions are given for diffractive processes at Tevatron and LHC. Stringent tests of our model and of its parameters using data being taken now at Tevatron Run II are suggested. These measurements will also allow to discriminate between various models and finally to give precise predictions on diffractive Higgs boson production cross-section at the LHC.

  18. The Legacy of the Tevatron in the Area of Accelerator Science

    CERN Document Server

    Holmes, Stephen D

    2013-01-01

    For more than 25 years the Tevatron was the highest energy accelerator in the world, providing the first access to particle collisions beyond 1 TeV and achieving an ultimate performance a factor of four hundred beyond the original design goals. This article reviews the many formidable challenges that were overcome, and the knowledge gained, in building, operating, and improving the Tevatron over its lifetime. These challenges included: the first operations of an accelerator based on superconducting magnets, production of antiprotons in sufficient numbers to support a useable luminosity, management of beam-beam, intrabeam, and other collective effects, novel manipulations of the beam longitudinal phase space, and development and application of a wide variety of innovative technologies. These achievements established the legacy of the Tevatron as the progenitor of all subsequently constructed high energy hadron colliders.

  19. La mesure du danger

    CERN Document Server

    Manceron, Vanessa; Revet, Sandrine

    2014-01-01

    La mesure du danger permet d’explorer des dangers de nature aussi diverse que la délinquance, la pollution, l’écueil maritime, la maladie ou l’attaque sorcellaire, l’extinction d’espèces animales ou végétales, voire de la Planète tout entière. Au croisement de la sociologie, de l’anthropologie et de l’histoire, les différents articles analysent les pratiques concrètes de mesure pour tenter de comprendre ce qui se produit au cours de l’opération d’évaluation du danger sans préjuger de la nature de celui-ci. L’anthropologie a contribué à la réflexion sur l’infortune en s’intéressant aux temporalités de l’après : maladies, catastrophes, pandémies, etc. et en cherchant à rendre compte de l’expérience des victimes, de leur vie ordinaire bouleversée, de la recomposition du quotidien. Elle s’intéresse aussi aux autres types de mesures, les savoirs incorporés, qui reposent sur l’odorat, la vue ou le toucher et ceux qui ressortent d’une épistémologie « non ...

  20. Har du sikret din alderdom?

    DEFF Research Database (Denmark)

    Kiens, Bente; Aagaard, Peter Gjerndrup

    2006-01-01

    Daglig fysisk aktivitet kan betragtes som indbetaling op din personlige helbredspension. Jo mere du sætter ind på kontoen, og jo oftere du gør det, jo større er sandsynligheden for, at du lever længere og får et sundere helbred. Og det er aldrig for sent at starte med indbetalingerne....

  1. L’invitation au marriage. Une approche des réseaux de sociabilité du couple.

    Directory of Open Access Journals (Sweden)

    Maillochon, F.

    2009-06-01

    Full Text Available Cet article décrit les enjeux sociaux de l’élaboration de la liste d’invités aux cérémonies de mariage. Cette circonstance constitue une opportunité rare pour le sociologue d’observer un « réseau de sociabilité » objectivé par les acteurs eux-mêmes. La mise en regard du contenu effectif de ces listes avec les discours recueillis auprès des couples sur les logiques et les hésitations ayant présidé à leurs choix permet de nuancer le caractère substantialiste qui est souvent attribué aux « réseaux ». Inviter quelqu’un à son mariage n’est pas une simple opération de mise à plat de ses relations amicales, mais une action performatrice qui permet de les construire et de les projeter dans l’avenir. L’invitation au mariage semble aussi largement conditionnée par les positions sociales respectives des personnes concernées de sorte que reconnaissance affective et reconnaissance sociale apparaissent souvent indissociables dans l’élaboration de cette relation. Les invités au mariage ne représentent donc pas seulement un état de fait du réseau amical produit par l’histoire du couple et inscrit dans le passé de chacun, mais aussi une promesse sur l’évolution du rayonnement affectif, mais aussi social, de celui-ci.

  2. Top quark mass: Latest CDF results, Tevatron combination and electroweak implications

    Energy Technology Data Exchange (ETDEWEB)

    Vellidis, Costas

    2009-10-01

    A summary of the most up-to-date top quark mass measurements at CDF is presented. These analyses use top-antitop candidate events detected in the CDF experiment at the Tevatron collider with an integrated luminosity of up to {approx}3/fb. The combination of all those measurements together with the corresponding top mass measurements from the concurrently running D0 experiment at the Tevatron yields a world average of M{sub t} = [173.1 {+-} 0.6(stat.) {+-} 1.1(syst.)] GeV/c{sup 2}.

  3. Contributions to the mini-workshop on beam-beam compensation in the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Shiltsev, V.

    1998-02-01

    The purpose of the Workshop was to assay the current understanding of compensation of the beam-beam effects in the Tevatron with use of low-energy high-current electron beam, relevant accelerator technology, along with other novel techniques of the compensation and previous attempts. About 30 scientists representing seven institutions from four countries--FNAL, SLAC, BNL, Novosibirsk, CERN, and Dubna were in attendance. Twenty one talks were presented. The event gave firm ground for wider collaboration on experimental test of the compensation at the Tevatron collider. This report consists of vugraphs of talks given at the meeting.

  4. Study of the linked dipole chain model in heavy quark production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Lipatov, Artem V. [Physical Department, M.V. Lomonosov Moscow State University, Moscow (Russian Federation)]. E-mail: lipatov@theory.sinp.msu.ru; Leif Loennblad [Dept. of Theoretical Physics, Lund (Sweden)]. E-mail: Leif.Lonnblad@thep.lu.se; Zotov, Nikolai P. [D.V. Skobeltsyn Institute of Nuclear Physics, M.V. Lomonosov Moscow State University, Moscow (Russian Federation)]. E-mail: zotov@theory.sinp.msu.ru

    2004-01-01

    We present calculations of charm and beauty production at Tevatron within the framework of k{sub T} -factorization, using the unintegrated gluon distributions as obtained from the Linked Dipole Chain model. The analysis covers transverse momentum and rapidity distributions and the azimuthal correlations between b and b-bar quarks (or rather muons from their decay) which are powerful tests for the different unintegrated gluon distributions. We compare the theoretical results with recent experimental data taken by D{phi} and CDF collaborations at the Tevatron Run I and II. (author)

  5. Multiple Parton Interactions in ppbar Collisions in D0 Experiment at the Tevatron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Golovanov, Georgy [Dubna, JINR

    2016-01-01

    The thesis is devoted to the study of processes with multiple parton interactions (MPI) in a ppbar collision collected by D0 detector at the Fermilab Tevatron collider at sqrt(s) = 1.96 TeV. The study includes measurements of MPI event fraction and effective cross section, a process-independent parameter related to the effective interaction region inside the nucleon. The measurements are done using events with a photon and three hadronic jets in the final state. The measured effective cross section is used to estimate background from MPI for WH production at the Tevatron energy

  6. Search For Magnetic Monopoles Possibly Produced By Proton-antiproton Collisions At The Tevatron Collider

    CERN Document Server

    Luo, W

    2002-01-01

    Magnetic monopoles can be used to explain the quantization of electric charge, and are predicted by gauge field theory. If monopoles exist, they could have been produced by the proton-antiproton collisions at the Tevatron collider—the highest energy accelerator existing in the world, and trapped in the CDF and DØ detectors. We took Al, Be, and Pb samples from the Tevatron and used the induction technique with SQUIDs (Superconducting Quantum Interference Devices) to detect monopoles in the samples. We did not find monopoles, but we have set new limits for the monopole mass and the relavant cross section based on a Drell-Yan model and Monte Carlo calculation.

  7. L’effet du style d’apprentissage sur la mémoire transactive d’équipes collaboratives en formation à distance

    Directory of Open Access Journals (Sweden)

    Sandrine Decamps

    2012-01-01

    Full Text Available L’objectif de cette contribution est d’étudier l’effet du style d’apprentissage sur le système de mémoire transactive d’équipes collaboratives. Pour ce faire, trois modalités de constitution d’équipes ont été expérimentées auprès de 126 apprenants impliqués dans deux activités collectives. L’analyse du système de mémoire transactive révèle une influence positive de la modalité de constitution d’équipes. Le fait de constituer des équipes équilibrées en tenant compte du style d’apprentissage participatif favorise chez l’apprenant une meilleure perception de la spécialisation et de la crédibilité de ses coéquipiers.

  8. Les pirogues du Maroni

    Directory of Open Access Journals (Sweden)

    Sophie François

    2012-04-01

    Full Text Available Sur le Maroni, fleuve frontière entre la Guyane française et le Surinam, les pirogues amarrées le long des berges se comptent par centaines. Elles représentent le seul moyen de transport pour les milliers de personnes vivant sur les rives du Maroni. Les différentes formes de pirogues sont révélatrices de la diversité géographique du Maroni et de la diversité culturelle des populations. Les Amérindiens du littoral naviguent uniquement dans l’estuaire du fleuve. Ils construisent des pirogues larges, hautes et terminées à la poupe par une haute étrave qui fend les vagues. Ces pirogues sont construites à partir d’une coque monoxyle expansée et rehaussée d’un ou de deux bordages. En chauffant la grume évidée, le bois acquiert une certaine plasticité qui permet d’écarter les flancs et d’obtenir une coque très large à partir d’un arbre de faible diamètre. Les Bushinenge, populations d’origine africaine qui ont déserté les grandes plantations de la Guyane hollandaise dès le début du XVIIe siècle et se sont installées sur les deux rives du Maroni, ont développé des formes de pirogues adaptées au passage des sauts. Leurs pirogues, construites également en expansant la coque au feu, sont étroites et longues et possèdent des extrémités curvilignes qui dépassent largement au–dessus du bordage. Les longues pirogues à moteur comme les canots–pagaies sont ornés de motifs d’entrelacs appelés tembé ; et de décors d’inspiration contemporaine. L’inventaire des pirogues du Maroni a mis en évidence la richesse et la vitalité du patrimoine nautique de cette région au début du XXIe siècle, tant au niveau des formes des embarcations que des décors et des pratiques de navigation.On the Maroni river, natural border between French Guyana and the Surinam, canoes tied to the river banks can be counted by the hundreds. They are the only mean of transportation for thousands of people living along the

  9. L'entreprise face à la biodiversité : le cas de l'entreprise brésilienne NATURA et son partenariat avec les extraxtivistes de la " réserve de développement durable du fleuve Iratapuru " dans la region de Jarí , Amazonie brésilienne

    OpenAIRE

    Greissing, Anna; Le Tourneau, François-Michel; Kohler, Florent; Picanço, José Reinaldo Alves

    2008-01-01

    Les actes de la conférence sont en attente d'apparition. L'ouvrage est coordonné par Sylvie Daviet, Université de Provence (Aix-Marseille).; International audience; La " réserve de développement durable " du fleuve Iratapuru est exploitée par la communauté de São Francisco. Du fait de ses efforts pour s'organiser et pour améliorer les conditions de vie de ses habitants, ce village est petit à petit devenu un symbole des efforts de développement réalisés auprès des " communautés traditionnelle...

  10. L'Origine du Monde

    CERN Multimedia

    CNET & Ecole Polytechnique Paris; Vincent Ferreira

    1996-01-01

    Création, théologie, science, découverte, recherche, religion, condition humaine.Avec Maurice Jacob physicien, Hubert Curien Président du Conseil du CERN, Michael Doser physicien, Frère Emile Communauté de Taizé.

  11. discours du Directeur General

    CERN Document Server

    CERN. Geneva

    2007-01-01

    L'année 2007 est une année très spéciale pour le CERN. Je vous propose de nous retrouver pour faire le point sur les activités en cours. Rendez-vous le mercredi 27 juin à 15h00 dans l'amphithéâtre principal. La transmission simultanée sera assurée dans les amphithéâtres IT, AT, AB Prevessin et dans la Salle du Conseil. Robert Aymar

  12. Electroweak radiative effects in the single $W$-production at Tevatron and LHC

    CERN Document Server

    Akushevich, I; Shumeiko, N M; Zykunov, V A

    2003-01-01

    An alternative calculation of the lowest order electroweak radiative corrections to the single W-boson production in hadron-hadron collision in the framework of the quark parton model without any absorption of the collinear quark singularity into the parton distributions is carried out. Numerical analysis under Tevatron and LHC kinematic conditions is performed.

  13. Exclusive e+e-, di-photon and di-jet production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Terashi, Koji; /Rockefeller U.

    2007-05-01

    Results from studies on exclusive production of electron-position pair, di-photon, and dijet production at CDF in proton-antiproton collisions at the Fermilab Tevatron are presented. THe first observation and cross section measurements of exclusive e{sup +}e{sup -} and di-jet production in hadron-hadron collisions are emphasized.

  14. B_s oscillation and prospects for delta m_s at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Menzemer, Stephanie; /MIT

    2005-07-01

    Till the start of the LHC, the Tevatron is the only running accelerator which produces enough B{sub s} mesons to perform {Delta}m{sub s} measurements. The status--as it was at the time of the conference--of two different {Delta}m{sub s} analysis performed both by the CDF and D0 collaboration will be presented.

  15. Direct photon production in NCG QCD at the tevatron and LHC

    Energy Technology Data Exchange (ETDEWEB)

    Bekli, M. R.; Mebarki, N.; Chadou, I. [Laboratoire de Physique Mathematique et Subatomique, Mentouri University, Constantine (Algeria)

    2012-06-27

    The minimal NCSM contribution of a direct photon production at the Tevatron and LHC is obtained and the phenomenological implications are discussed. Some behaviors are discussed. It is shown that the effect of the space-time noncommutativity becomes important at very high energies leading to a violation of unitarity.

  16. Improving the discovery potential of charged Higgs bosons at the Tevatron and large hadron collider

    Indian Academy of Sciences (India)

    Stefano Moretti

    2003-02-01

    We outline several improvements to the experimental analyses carried out at Tevatron (Run 2) or simulated in view of the large hadron collider (LHC) that could increase the scope of CDF/D0 and ATLAS/CMS in detecting charged Higgs bosons.

  17. Accelerator Science and Technology Breakthroughs, Achievements and Lessons from the Tevatron

    CERN Document Server

    Shiltsev, Vladimir

    2011-01-01

    For almost a quarter of a century, the Tevatron proton-antiproton collider was the centerpiece of the world's high energy physics program - beginning operation in December of 1985 until it was overtaken by LHC in 2011. The aim of this unique scientific instrument was to explore the elementary particle physics reactions with center of mass collision energies of up to 1.96 TeV. The initial design luminosity of the Tevatron was 1030cm-2s-1, however as a result of two decades of upgrades, the accelerator has been able to deliver 430 times higher luminosities to each of two high luminosity experiments, CDF and D0. The Tevatron will be shut off September 30, 2011. The collider was arguably one of the most complex research instruments ever to reach the operation stage and is widely recognized for many technological breakthroughs and numerous physics discoveries. In this John Adams lecture, I briefly present the history of the Tevatron, major advances in accelerator physics, and technology implemented during the long...

  18. The upgraded data acquisition system for beam loss monitoring at the Fermilab Tevatron and Main Injector

    CERN Document Server

    Baumbaugh, A; Brown, B C; Capista, D; Drennan, C; Fellenz, B; Knickerbocker, K; Lewis, J D; Marchionni, A; Needles, C; Olson, M; Pordes, S; Shi, Z; Still, D; Thurman-Keup, R; Utes, M; Wu, J

    2011-01-01

    A VME-based data acquisition system for beam-loss monitors has been developed and is in use in the Tevatron and Main Injector accelerators at the Fermilab complex. The need for enhanced beam-loss protection when the Tevatron is operating in collider-mode was the main driving force for the new design. Prior to the implementation of the present system, the beam-loss monitor system was disabled during collider operation and protection of the Tevatron magnets relied on the quench protection system. The new Beam-Loss Monitor system allows appropriate abort logic and thresholds to be set over the full set of collider operating conditions. The system also records a history of beam-loss data prior to a beam-abort event for post-abort analysis. Installation of the Main Injector system occurred in the fall of 2006 and the Tevatron system in the summer of 2007. Both systems were fully operation by the summer of 2008. In this paper we report on the overall system design, provide a description of its normal operation, and...

  19. Les risques du travail

    CERN Document Server

    Thébaud-Mony, Annie

    2015-01-01

    Depuis les années 1990, les conditions de travail se sont peu à peu imposées dans le débat social. Néanmoins, la situation reste critique. Les risques traditionnels n'ont pas disparu : les manutentions lourdes, l'exposition professionnelle aux cancérogènes, au bruit ou aux vibrations demeurent répandues... De plus, certaines " améliorations " n'ont fait que déplacer et dissimuler les problèmes, telle l'externalisation des risques grâce à la sous-traitance. Dans le même temps, les transformations du travail et des modalités de gestion de la main-d'œuvre ont fragilisé les collectifs et accru l'isolement des salariés, conduisant à une montée visible de la souffrance psychique. Face à ces évolutions, il est plus que jamais nécessaire que tous les acteurs concernés, en particulier les salariés eux-mêmes et leurs représentants, s'approprient les connaissances indispensables pour améliorer la protection de la santé sur les lieux du travail. Tel est le but de ce livre, qui renouvelle int�...

  20. Search for the first generation scalar leptoquarks with D0; Recherche de leptoquarks scalaires de premiere generation aupres de D0

    Energy Technology Data Exchange (ETDEWEB)

    Cothenet, A

    2004-05-15

    This work was dedicated to the search for pairs of first generation scalar leptoquarks one decaying into ej and the other into {nu}j. The experimental data used (175,6 pb{sup -1}) is that collected during the run-II of the D0 experiment at Tevatron. The production cross-sections of scalar leptoquark pairs has been assessed at a 95% confidence level for different values of the mass. The comparison of these values with theoretical values has led us to state that for a branching ratio {beta} = 0.5 the existence of scalar leptoquarks with a mass lower than 194 GeV is not possible. For a branching ratio {beta} = 1, some scalar leptoquarks with mass < 238 GeV may be excluded while for {beta} = 0.5, some scalar leptoquarks with mass < 213 GeV are excluded.

  1. Jouer du piano

    Directory of Open Access Journals (Sweden)

    Fériel Kaddour

    2011-04-01

    Full Text Available La réflexion s’appuie dans un premier temps sur une opposition entre deux attitudes de pianistes  à l’égard du travail à l’instrument : Gould, qui revendique une séparation d’avec le clavier pour ne privilégier que la lecture; Arrau, dont la technique au contraire vise à « faire corps » avec son piano. L’étude de ces deux démarches d’interprètes conduit à une conclusion croisée : l’abstraction gouldienne n’est rien d’autre qu’un déplacement du jeu vers d’autres instruments (ceux qui servent à la prise de son et au montage de ses enregistrements ; le « faire-corps » hérité de la culture pianistique romantique est plus dialectique que fusionnel, et en cela implique une capacité de mise à distance. A partir de cette double conclusion, on tâche enfin de repenser la place du jeu à l’instrument dans la mise en œuvre d’une interprétation, en interrogeant le dialogue qui s’instaure entre la partition telle qu’elle s’écrit et le geste tel qu’il se joue.Our study leans on an opposition between two pianists' attitudes about their work with the instrument. Gould claims a necessary separation from the keyboard in order to prioritize reading. Arrau, on the contrary, relies on a technique which consists in “being one” with his piano. The analysis of these two interprets’ behaviours leads to a crossed conclusion: the gouldian abstraction is nothing else than a displacement of the playing towards another kind of instruments, the ones he uses in sound recording and cut up; Arrau’s “being one” is more dialectic than at first sight, and it therefore implies a real distancing from the piano. This constatation leads to rethink the place of the piano playing in the setting of an interpretation, and to highlight the real dialogue which develops itself between the score as it has been written and the gesture as it is played.

  2. Le sacre du printemps

    Directory of Open Access Journals (Sweden)

    Denise Pumain

    2002-03-01

    Full Text Available Cybergeo aura six ans en avril : dans la réalité du virtuel, dans l'univers récent et fluctuant de la publication en ligne, cela fait de nous, tout à la fois, des pionniers et des vétérans. De façon plus surprenante, il se trouve que nous sommes aussi uniques : parmi toutes les revues électroniques de sciences sociales, aucune ne combine comme Cybergeo ancienneté, publication exclusivement électronique, liberté d'accès au texte intégral, édition et gestion par des chercheurs, et comité de lec...

  3. OPERATION DU FOISONNEMENT

    Directory of Open Access Journals (Sweden)

    Gholamreza Djelveh

    2010-04-01

    Full Text Available Mousses alimentaires sont un sous-ensemble des aliments connus sous le nom de produits fouettés ou des produits aérés. Ils sont des produits formulés avec des qualités telles que la légèreté et la souplesse et sont principalement consommés à l'apéritif ou au dessert. Les produits en mousse obtenue par dispersion d'un gaz dans une matrice alimentaire (la phase continue ont connu un développement croissant au cours des années 80 et 90. Le processus d'aération liés à leurs activités de production est appelée l'expansion ou à fouetter. Le document présente les principaux-paramètres du procédé du point permanent de la formulation, la mise en œuvre processus dans les installations pilotes et à l'échelle industrielle, la caractérisation des produits finis, la base énergétique de l'échelle de processus en place, et le lien entre la formulation, émulsion préparation de l'expansion. Cette vue d'ensemble de l'opération d'expansion continue, nous a permis de mettre en évidence le fait qu'il ya des opérations de l'unité encore mal décrite par le génie des procédés et pour lesquels les méthodes et outils pour l'extrapolation et la prédiction sont encore à leurs balbutiements.

  4. Les accrédités auprès de l’UE et les correspondants français et italiens face au défi numérique

    Directory of Open Access Journals (Sweden)

    Antonella Agostino

    2016-09-01

    Full Text Available Dans un contexte dominé par l’immédiateté et la multiplication des sources d’information et les outils du Web 2.0, les médias sociaux sont devenus incontournables dans la production et le traitement de l’actualité internationale. Le présent article se propose de déterminer les conséquences de cette nouvelle configuration sur la production de l’information européenne et sur l’évolution du poste de correspondant accrédité auprès de l’Union européenne, en nous intéressant spécifiquement aux français et italiens, pour lesquels aucune recherche n’a été publiée jusqu’à présent. Notre investigation, basée notamment sur des enquêtes de terrain, des statistiques et des analyses d’entretiens semi-directifs, tente de répondre aux questions suivantes : l’Internet et les médias sociaux, exploités prioritairement par les institutions européennes, représentent-t-ils pour l’accrédité un nouvel outil de travail et un nouveau terrain d’expression et de diffusion de l’information ? Ces médias bouleversent-ils leurs pratiques ? Quelle est l’attitude des accrédités face à l’essor du journalisme amateur ? Quel est l’impact du web social sur leur statut de news-gatherer et news-manufacturer ? Nos observations montrent que l’irruption du numérique ne semble pas avoir suscité une véritable réorganisation en profondeur des structures de production ni même des routines de travail de l’accrédité : le Web 2.0 représente une source d’information complémentaire des sources traditionnelles. Dans le microcosme bruxellois, certains s’adressent à leurs sources confidentielles ou appellent un collègue pour vérifier une information, d’autres surfent à la recherche d’un scoop et considèrent la toile comme un nouveau moyen pour mieux vendre la news « Europe ». Même s’il est devenu possible aujourd’hui pour de nouveaux acteurs opérant en ligne de suivre l’actualité et la

  5. HIGH-pT Features of z-SCALING at Rhic and Tevatron

    Science.gov (United States)

    Tokarev, M. V.; Zborovsky, I.; Dedovich, T. G.

    2008-09-01

    Experimental data on inclusive cross sections of jet, direct photon, and high-pT hadron production in pp/bar pp and AA collisions are analyzed in the framework of z-scaling. The analysis is performed with data obtained at ISR, Sbar ppS, RHIC, and Tevatron. Scaling properties of z-presentation of the inclusive spectra are verified. Physical interpretation of the variable z and the scaling function ψ(z) is discussed. We argue that general principles of self-similarity, locality, and fractality reflect the structure of the colliding objects, interaction of their constituents, and particle formation at small scales. The obtained results suggest that the z-scaling may be used as a tool for searching for new physics phenomena beyond Standard Model in hadron and nucleus collisions at high transverse momentum and high multiplicity at U70, RHIC, Tevatron, and LHC.

  6. CMS Pixel Telescope Addition to T-980 Bent Crystal Collimation Experiment at the Tevatron

    CERN Document Server

    Rivera, Ryan; Johnson, Todd; Kwan, Simon; Lundberg, Carl; Still, Dean; Prosser, Alan; Uplegger, Lorenzo; Zagel, Jim; Zvodaya, Viktoriya

    2012-01-01

    An enhancement to the T-980 bent crystal collimation experiment at the Tevatron has been completed. The enhancement was the installation of a pixel telescope inside the vacuum-sealed beam pipe of the Tevatron. The telescope is comprised of six CMS PSI46 pixel plaquettes, arranged as three stations of horizontal and vertical planes, with the CAPTAN system for data acquisition and control. The purpose of the pixel telescope is to measure beam profiles produced by bent crystals under various conditions. The telescope electronics inside the beam pipe initially were not adequately shielded from the image current of the passing beams. A new shielding approach was devised and installed, which resolved the problem. The noise issues encountered and the mitigating techniques are presented herein, as well as some preliminary results from the telescope.

  7. Studies of top quark properties and search for electroweak single top quark production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Datta, Mousumi; /Fermilab

    2007-10-01

    The top quark was discovered in 1995 by the CDF and D0 experiments at the Fermilab Tevatron during the Run I operation. Since the start of the Tevatron Run II in 2001, both experiments have collected {approx}2 fb{sup -1} data samples, which are over twenty times larger than that used in the Run 1 discovery. This larger data sample allows more precise studies of top-quark properties; differences between observed top-quark properties and the Standard Model (SM) prediction may give hints to possible physics beyond the SM. Here we present the latest results on the measurements of top-quark properties and the search for electroweak (EW) single top quark production from the CDF and D0 collaborations. The integrated luminosity used for the measurements corresponds to about 1 fb{sup -1}.

  8. Tevatron Top-Quark Combinations and World Top-Quark Mass Combination

    Energy Technology Data Exchange (ETDEWEB)

    Peters, Reinhild Yvonne [DESY

    2014-11-04

    Almost 20 years after its discovery, the top quark is still an interesting particle, undergoing precise investigation of its properties. For many years, the Tevatron proton antiproton collider at Fermilab was the only place to study top quarks in detail, while with the recent start of the LHC proton proton collider a top quark factory has opened. An important ingredient for the full understanding of the top quark is the combination of measurements from the individual experiments. In particular, the Tevaton combinations of single top-quark cross sections, the ttbar production cross section, the W helicity in top-quark decays as well as the Tevatron and the world combination of the top-quark mass are discussed.

  9. Measurement of Beam Tunes in the Tevatron Using the BBQ System

    Energy Technology Data Exchange (ETDEWEB)

    Edstrom, Dean R.; /Indiana U.

    2009-04-01

    Measuring the betatron tunes in any synchrotron is of critical importance to ensuring the stability of beam in the synchrotron. The Base Band Tune, or BBQ, measurement system was developed by Marek Gasior of CERN and has been installed at Brookhaven and Fermilab as a part of the LHC Accelerator Research Program, or LARP. The BBQ was installed in the Tevatron to evaluate its effectiveness at reading proton and antiproton tunes at its flattop energy of 980 GeV. The primary objectives of this thesis are to examine the methods used to measure the tune using the BBQ tune measurement system, to incorporate the system into the Fermilab accelerator controls system, ACNET, and to compare the BBQ to existing tune measurement systems in the Tevatron.

  10. CMS Pixel Telescope Addition to T-980 Bent Crystal Collimation Experiment at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Rivera, Ryan; Annala, Jerry; Johnson, Todd; Kwan, Simon; Lundberg, Carl; Still, Dean; Prosser, Alan; Uplegger, Lorenzo; Zagel, Jim; Zvodaya, Viktoriya; /Fermilab

    2011-09-14

    An enhancement to the T-980 bent crystal collimation experiment at the Tevatron has been completed. The enhancement was the installation of a pixel telescope inside the vacuum-sealed beam pipe of the Tevatron. The telescope is comprised of six CMS PSI46 pixel plaquettes, arranged as three stations of horizontal and vertical planes, with the CAPTAN system for data acquisition and control. The purpose of the pixel telescope is to measure beam profiles produced by bent crystals under various conditions. The telescope electronics inside the beam pipe initially were not adequately shielded from the image current of the passing beams. A new shielding approach was devised and installed, which resolved the problem. The noise issues encountered and the mitigating techniques are presented herein, as well as some preliminary results from the telescope.

  11. Tevatron constraint on the Kaluza-Klein gluon of the Bulk Randall-Sundrum model

    CERN Document Server

    Guchait, M; Sridhar, K

    2007-01-01

    The Bulk Randall-Sundrum model, where all Standard Model particles except the Higgs are free to propagate in the bulk, predicts the existence of Kaluza-Klein (KK) modes of the gluon with a large branching into top-antitop pairs. We study the production of the lowest KK gluon mode at the Tevatron energy and use the data on the top cross-section from the Run II of Tevatron to put a bound on the mass of the KK gluon. The resulting bound of 800 GeV, while being much smaller than the constraints obtained on the KK gluon mass from flavour-changing neutral currents, is the first, direct collider bound which is independent of the specificities of the model.

  12. Simulations of octupole compensation of head-tail instability at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Meiqin Xiao; Tanaji Sen; Frank Schmidts

    2003-05-28

    The proton lifetime in the Tevatron depends sensitively on chromaticities. Too low chromaticities can make the beam unstable due to the weak head-tail instability. One way to compensate this effect is to introduce octupoles to create a larger amplitude dependent betatron tune spread. However, the use of octupoles will also introduce additional side effects such as second order chromaticity, differential tune shifts and chromaticities on both proton and anti-proton helices. The non-linear effects may also reduce the dynamic aperture. There are 67 octupoles in 4 different circuits in the Tevatron which may be used for this purpose. We report on a simulation study to find the best combinations of polarities and strengths of the octupoles.

  13. Health physics problems due to tritium around heavy-water reactors; Les problemes de radioprotection poses par le tritium aupres des piles a eau lourde

    Energy Technology Data Exchange (ETDEWEB)

    Chassany, J.; Roux, J.M. [Commissariat a l' Energie Atomique, Chusclan (France). Centre de Production de Plutonium de Marcoule

    1969-07-01

    A review is made, after one year operation, of the protection against tritium in a heavy-water reactor: - nature of the tritium risk, particular to this type of installation; - detection and measurement equipment; - working method; - results obtained concerning the supervision of the personnel, the installation, and the servicing operations. (authors) [French] Le bilan de la protection contre le tritium dans une pile a eau lourde, a l'issue d'une annee de fonctionnement, est presente: - nature du risque tritium specifique d'une telle installation; - moyens de detection et de mesure; - methode de travail; - resultats obtenus quant a la surveillance du personnel, de l'installation et des interventions. (auteurs)

  14. Intervenir auprès de familles vulnérables selon les principes de la théorie de l’attachement

    Directory of Open Access Journals (Sweden)

    Diane St-Laurent

    2008-01-01

    Full Text Available La maltraitance est considérée comme une perturbation sévère de la relation entre le parent et l’enfant qui entrave de façon importante le bon développement de ce dernier. Les enfants victimes de négligence ou de violence sont particulièrement à risque de développer des problèmes d’adaptation psychosociaux sérieux durant l’enfance et l’adolescence, tels des problèmes de comportement (anxiété, agressivité et des difficultés scolaires. La théorie de l’attachement et les travaux de recherche de ce domaine suggèrent que des stratégies d’intervention axées sur la qualité des interactions parent-enfant peuvent améliorer la relation d’attachement et ainsi contribuer à prévenir l’apparition de problèmes d’adaptation chez les enfants maltraités. Dans cet article, nous décrivons une intervention inspirée de la théorie de l’attachement qui a été implantée auprès de familles vulnérables ayant un jeune enfant maltraité ou à très haut risque de maltraitance. Il s’agit d’une intervention brève centrée sur l’observation des interactions parent-enfant et qui utilise la rétroaction vidéo avec le parent. Elle a pour objectif d’augmenter la sensibilité de ce dernier à l’égard des besoins et signaux de son enfant et d’améliorer la sécurité d’attachement de l’enfant. Les principes à la base de cette intervention sont exposés ainsi que les raisons qui ont guidé le choix des stratégies d’intervention.

  15. Di-J/psi production at the Tevatron and the LHC

    CERN Document Server

    Lansberg, Jean-Philippe

    2016-01-01

    We briefly review recent results which we have obtained in the study of J/psi-pair production at the Tevatron and the LHC. We claim that the existing data set from CMS and D0 point at a significant double-parton-scattering contribution with an effective cross section smaller than that for jet-related observables. We have also derived simple relations involving feed-down fractions from excited states which can help in disentangling the single from the double scatterings.

  16. Development of 3D beam-beam simulation for the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Stern, E.; Amundson, J.; Spentzouris, P.; Valishev, A.; /Fermilab; Qiang, J.; Ryne, R.; /LBL, Berkeley

    2007-06-01

    We present status of development of a 3D Beam-Beam simulation code for simulating the Fermilab Tevatron collider. The essential features of the code are 3D particle-in-cell Poisson solver for calculating the Beam-Beam electromagnetic interactions with additional modules for linear optics, machine impedance and chromaticity, and multiple bunch tracking. The simulations match synchrobetatron oscillations measured at the VEPP-2M collider. The impedance calculations show beam instability development consistent with analytic expressions.

  17. chi_{c1} and chi_{c2} decay angular distributions at the Fermilab Tevatron

    CERN Document Server

    Kniehl, Bernd A; Palisoc, C P

    2003-01-01

    We consider the hadroproduction of chi_{c1} and chi_{c2} mesons and their subsequent radiative decays to J/psi mesons and photons in the factorization formalism of nonrelativistic quantum chromodynamics, and study the decay angular distributions, by means of helicity density matrices, in view of their sensitivity to color-octet processes. We present numerical results appropriate for the Fermilab Tevatron.

  18. Dijets with 2,1 or 0 rapidity gap: Factorization breaking at the Tevatron

    CERN Document Server

    Bialas, A

    2003-01-01

    Central production cross-sections of hard dijets with 2,1 or 0 rapidity gap at Tevatron are analyzed in terms of diffractive (``a la Good-Walker'') and non diffractive fluctuations of the incident particles. The observed large factorization breaking and the unexpected high value of the 2 to 1 gap cross-section ratio are explained in terms of scattering with and between the incident particles.

  19. Phenomenological study of the atypical heavy flavor production observed at the Fermilab Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Apollinari, G.; Barone, M.; Fiori, I.; Giromini, P.; Happacher, F.; Miscetti, S.; Parri, A.; Ptohos, F.; /Frascati /Fermilab /INFN, Pisa /Cyprus U.

    2005-11-01

    The authors address known discrepancies between the heavy flavor properties of jets produced at the Tevatron collider and the prediction of conventional-QCD simulations. In this study, they entertain the possibility that these effects are real and due to new physics. They show that all anomalies can be simultaneously fitted by postulating the additional pair production of light bottom squarks with a 100% semileptonic branching fraction.

  20. Di-boson production and SM SUSY Higgs searches at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Elvira, V.Daniel; /Fermilab

    2005-07-01

    The discovery of the Higgs boson would be a major success for the Standard Model (SM) and would provide further insights into the electroweak symmetry breaking mechanism. This report contains the latest results from the D0 and CDF Tevatron experiments on searches for the SM Higgs produced from gluon fusion with H {yields} WW, and in association with a W boson. It also includes searches for a supersymmetric Higgs in the b{bar b} and {tau}{sup +}{tau}{sup -} decay channels. The study of di-boson production at the Tevatron is important to understand backgrounds in high mass Higgs searches. It also provides a test of the SM through the measurement of the production cross section and the gauge boson self couplings. This paper includes measurements of the WW, W{gamma}, and WZ production cross sections, as well as limits on the anomalous couplings associated with the WW{gamma} and WWZ interactions. The results are based on sets of up to 320 pb{sup -1} of data collected by the D0 and CDF experiments at the {bar p}p Tevatron collider, running at a center-of-mass energy of 1.96 TeV.

  1. Searches for the Standard Model Higgs boson at the Tevatron collider

    Science.gov (United States)

    Fisher, Wade C.; Junk, Thomas R.

    2016-10-01

    During Run II of the Tevatron collider, which took place from 2001 until 2011, the CDF and D0 detectors each collected approximately 10 fb -1 of poverline p collision data at a center-of-mass energy of √ s = 1.96 TeV. This dataset allowed for tests for the presence of the SM Higgs boson in the mass range 90-200 GeV in the production modes gg → H, W/ZH, vector-boson fusion, and toverline tH, with H decay modes H → boverline b, H → W+W-, H → τ+τ-, H → γγ, and H → ZZ. This chapter summarizes the search methods and the results of the Higgs boson search at the Tevatron. The increased sophistication of the analysis techniques as the collider run progressed is discussed, covering the strategies used over time to improve the sensitivity and breadth of the analyses. Using the full Tevatron data sample for both experiments, the combined Higgs search in all channels observes an excess consistent with the predicted SM Higgs boson signal with mass of 125 GeV, with a significance of 3.0 standard deviations above the background prediction.

  2. A 6kV Arbitrary Waveform Generator for the Tevatron Lens

    CERN Document Server

    Pfeffer, H; 10.1088/1748-0221/6/11/P11003

    2012-01-01

    This paper reports on a 6 kV modulator built and installed at Fermilab to drive the electron gun anode for the Tevatron Electron Lens (TEL). The TEL was built with the intention of shifting the individual (anti)proton bunch tunes to even out the tune spread among all 36 bunches with the desire of improving Tevatron integrated luminosity. This modulator is essentially a 6 kV arbitrary waveform generator that enables the TEL to define the electron beam intensity on a bunch-by-bunch basis. A voltage waveform is constructed having a 7 {\\mu}s duration that corresponds to the tune shift requirements of a 12-bunch (anti)proton beam pulse train. This waveform is played out for any one or all three bunch trains in the Tevatron. The programmed waveform voltages transition to different levels at time intervals corresponding to the 395 ns bunch spacing. Thus, complex voltage waveforms can be played out at a sustained rate of 143 kHz over the full 6 kV output range. This paper describes the novel design of the inductive a...

  3. Tevatron Higgs Mass Bounds: Projecting U(1)' Models to LHC Domain

    CERN Document Server

    Sert, Hale; Demir, Durmus A; Solmaz, Levent

    2010-01-01

    We study Higgs boson masses in supersymmetric models with an extra U(1) symmetry to be called U(1)$^{\\prime}$. Such extra gauge symmetries are urged by the $\\mu$ problem of the MSSM, and they also arise frequently in low-energy supersymmetric models stemming from GUTs and strings. We analyze mass of the lightest Higgs boson and various other particle masses and couplings by taking into account the LEP bounds as well as the recent bounds from Tevatron experiments. We find that the $\\mu$-problem motivated generic low-energy U(1)$^{\\prime}$ model yields Higgs masses as large as $\\sim 200\\ {\\rm GeV}$ and violate the Tevatron bounds for certain ranges of parameters. We analyze correlations among various model parameters, and determine excluded regions by both scanning the parameter space and by examining certain likely parameter values. We also make educated projections for LHC measurements in light of the Tevatron restrictions on the parameter space. We further analyze certain benchmark models stemming from E(6) ...

  4. Hiérophanie et sotériologie dans les traditions ismaéliennes du sous-continent indo-pakistanais

    Directory of Open Access Journals (Sweden)

    Michel Boivin

    2009-05-01

    Full Text Available Vers 1845, Hasan 'Alî Shâh, le guide divin (imam des Ismaéliens, trouva refuge dans le sous-continent indien. Auprès de ses disciples indiens, les Khojâhs, il exalta sa filiation avec l'imam Husayn pour légitimer son statut de sauveur, favorisant ainsi le développement des rituels shiites liés à Moharram. Son successeur 'Alî Shâh poursuivit cette œuvre avec la création du culte d'Amîr Pîr, où il essayait de marquer l'identité propre des Ismaéliens. Enfin, Sultân Muhammad Shâh éradiqua tous les intercesseurs pour se présenter comme le qâ'im, un sauveur individuel accessible à tous ici et maintenant.Dans la littérature religieuse des Khojâhs (ginân-s, bien que 'Alî soit présenté comme le mahdi, l'imam est qualifié de Naklankî, nom du 10e avatar de Vishnû, dont la parousie, chez les Hindous, est encore à venir. En revanche, chez les Ismaéliens de tradition persane du nord du Pakistan, l'imam est le qâ'im qui sauve les croyants individuellement, cet acte constituant une condition pour participer à la Résurrection orchestrée par le mahdi, le premier imam 'Alî. Les Ismaéliens ont par conséquent fait passer au premier plan le salut spirituel, alors que la Résurrection finale est reléguée dans un temps indéterminé.

  5. Le collisionneur du futur?

    CERN Multimedia

    CERN Audiovisual Service

    2009-01-01

    Pourquoi deux études parallèles pour un même collisionneur linéaire ? Loin d’être un double effort et un gaspillage de ressources, ces deux études s’inscrivent dans une stratégie de complémentarité afin de fournir la meilleure technologie requise par la physique du futur. Vendredi 12 juin a eu lieu au CERN la première réunion conjointe CLIC et ILC. Elle n’a pas été avare de bons résultats et d’importantes décisions. Le Collisionneur Linéaire International (ILC) et le Collisionneur Linéaire Compact (CLIC) sont deux études qui font, tous deux, appel à des technologies de pointe. A première vue en compétition, les deux études sont en réalité complémentaires et elles ont un objectif commun : proposer dans les plus brefs délais et au moindre coût, l‘accélérateur linéaire le mieux adapté pour prendre le relais de la physique des très hautes énergies après le LHC.

  6. Le bal du loup

    CERN Multimedia

    Happy Children's Home

    2013-01-01

    The Bord'eau amateur theatre group will graciously perform a play of their creation Le bal du loup Saturday 19 October 2013 at 20:00 Sunday 20 October at 17:00 in the Théâtre des Grottes Rue Louis Favre 43, 1201 Genève Children from age 12 upwards. Summary: The new-elected mayoress of a small village would like to clean up the town by prohibiting alcohol and getting rid of its prostitutes. Then along comes « Massimo Lupo » the pimp... The performances will be given to support the Happy Children's Home charity, which runs a foster-home in Pokhara for Nepali children:  http://www.happychildrenshome.org/ Admission : minimum charge of 10 CHF per person requested, to cover the cost of technical assistance and theatre rental. Any profit will be used solely for the foster-home. At the end of each performance members of the HCH charity will be happy to answer any questions you may have. The theatre has 86 seats, thank you for reserv...

  7. De nouveaux acteurs de la régulation du travail dans la gestion par projets

    Directory of Open Access Journals (Sweden)

    Marie-Josée Legault

    2009-03-01

    Full Text Available Dans le contexte d’une grande transformation de l’économie mondiale, on constate de plus en plus l’inadéquation des efforts de théorisation des relations de travail qui datent du fordisme, notamment du modèle d’analyse systémique (Dunlop, 1958 comme du modèle stratégique (Kochan, Katz et McKersie, 1986 ; dans ces deux modèles en effet, trois acteurs se partagent exclusivement la scène de l’action : les syndicats, les employeurs et l’État, et leurs interactions se déroulent essentiellement dans le cadre de l’État-nation. Or, on voit émerger de nouveaux modes de régulation qui, à leur tour, illustrent la nécessité d’intégrer de nouveaux acteurs et de nouvelles frontières aux modèles théoriques du système de relations industrielles. Une enquête menée auprès de 88 professionnels de l’informatique des entreprises de services technologiques aux entreprises, dans une population composée à parts égales d’hommes et de femmes, a permis d’y relever des pratiques de régulation qui non seulement remettent en cause les termes traditionnels de la régulation fordiste qui hier encore dominaient les bureaucraties professionnelles où on employait les professionnels de l’informatique, mais encore les frontières traditionnelles du système de relations industrielles selon deux aspects : celui des trois acteurs principaux : les employeurs, les travailleurs et l’État, par l’ajout du client et des équipes de travail ; et celui de la séparation entre les contextes du système de relations industrielles et ce système lui-même.As the global economy undergoes a major transformation, the inadequacy of labour relations theories dating back to Fordism, especially the systemic analysis model (Dunlop, 1958 and the strategic model (Kochan, Katz, & McKersie, 1986, in which only three actors—union, employer and State—share the stage is becoming increasingly obvious. A good example is provided by companies

  8. Study of a reconstruction algorithm for electrons in the ATLAS experiment in LHC; Etude d'un algorithme de reconstruction des electrons dans l'experience Atlas aupres du LHC

    Energy Technology Data Exchange (ETDEWEB)

    Kerschen, N

    2006-09-15

    The ATLAS experiment is a general purpose particle physics experiment mainly aimed at the discovery of the origin of mass through the research of the Higgs boson. In order to achieve this, the Large Hadron Collider at CERN will accelerate two proton beams and make them collide at the centre of the experiment. ATLAS will discover new particles through the measurement of their decay products. Electrons are such decay products: they produce an electromagnetic shower in the calorimeter by which they lose all their energy. The calorimeter is divided into cells and the deposited energy is reconstructed using an algorithm to assemble the cells into clusters. The purpose of this thesis is to study a new kind of algorithm adapting the cluster to the shower topology. In order to reconstruct the energy of the initially created electron, the cluster has to be calibrated by taking into account the energy lost in the dead material in front of the calorimeter. Therefore. a Monte-Carlo simulation of the ATLAS detector has been used to correct for effects of response modulation in position and in energy and to optimise the energy resolution as well as the linearity. An analysis of test beam data has been performed to study the behaviour of the algorithm in a more realistic environment. We show that the requirements of the experiment can be met for the linearity and resolution. The improvement of this new algorithm, compared to a fixed sized cluster. is the better recovery of Bremsstrahlung photons emitted by the electron in the material in front of the calorimeter. A Monte-Carlo analysis of the Higgs boson decay in four electrons confirms this result. (author)

  9. Measurement of the CP-violation parameter in the NA48 experiment in CERN installations; Mesure de la violation directe de CP aupres de l'experience NA48 du Cern

    Energy Technology Data Exchange (ETDEWEB)

    Granier de Cassagnac, R

    2000-05-11

    The experiment NA48 was mainly devoted to the measurement of the parameter characterizing the direct violation of CP: Re({epsilon}/{epsilon}'). The author has used experimental data that were collected in the second half of 1997, he proposed: Re({epsilon}/{epsilon}') (18.5 {+-} 4.5 (stat) {+-} 5.7 (syst)) * 10{sup -4}. This value is slightly lower than the average value (21.8 10{sup -4}) obtained over NA31, E731 experiments and the first results of kTeV and NA48 experiments. The first chapter proposes a didactical introduction to the concern of discrete symmetries in neutral kaons system. The second chapter presents the method chosen by the NA48 collaboration to perform the measurement of Re({epsilon}/{epsilon}') and the experimental equipment that is required. The third chapter is dedicated to the selection of events. The fourth chapter studies the efficiency of the trigger system for the events {pi}{sup +}{pi}{sup -} and {pi}{sup 0}{pi}{sup 0}. The fifth chapter presents the different corrections to bring to the experimental value in order to take into account the effects due to i) the tagging errors, ii) the background noise for {pi}{sup +}{pi}{sup -} and {pi}{sup 0}{pi}{sup 0} events, iii) the inaccuracy of triggers, iv) the change in detector acceptance according to the channels for K{sub s} or K{sub l} beams, v) the inaccuracy of the event reconstruction method, and vi) the unsteadiness of the intensity ratio K{sub s}/K{sub l}. (A.C.)

  10. ́Etude des états finals à deux bosons Z dans le canal leptons-neutrinos dans l'expérience CMS auprès du LHC au CERN

    CERN Document Server

    Marionneau, Matthieu

    2011-01-01

    This thesis presents a study of ZZ final states performed with data recorded with the CMS detector. This study exploits the first data delivered by the LHC and recorded by CMS in 2010 and 2011. The ZZ production cross section is measured and limits are set on neutral electroweak triple gauge couplings. The existence of such couplings would be an indication of new physics beyond the Standard Model. Moreover, the ZZ process in the Standard Model is a background for Higgs searches and have to be well known. Some preliminary studies are performed on the CMS electromagnetic calorimeter. These studies are related to the selective readout system and to the laser monitoring system of the electromagnetic calorimeter. The measurement and the behaviour of the transverse missing energy are also studied in events containing one electroweak boson decaying into electron(s). This study shows that pileup has a important effect on missing transverse energy measurements. Some corrections have to be taken into account to deal wi...

  11. Reconstruction des électrons et recherche de couplages anormaux dans le canal pp->ZZ->4l avec le détecteur CMS auprès du LHC

    CERN Document Server

    AUTHOR|(CDS)2075380; Charlot, Claude

    I did my PhD in Particle Physics with the CMS (Compact Muon Solenoid) team from Laboratoire Leprince-Ringuet at Ecole Polytechnique. The subjects of my study are the pp→ZZ+X production and the search for anomalous triple gauge couplings (ATGCs) using the data collected by the CMS detector at LHC at sqrt{s}=7 TeV. This work began with the first collisions at the LHC in the end of 2009 with the study and optimisation of electron reconstruction algorithms. Selection criteria of pure electrons samples from Z decays have been studied. The electron reconstruction efficiency has been measured on 2010 and 2011 data and the results have been used by the CMS collaboration for the 2010 and 2011 analyses. Then I dealt with the analysis of ZZ→4l channel and the search for anomalous triple gauge couplings, as possible signature of new physics. A recovery algorithm to correct the 4-leptons mass from Final State Radiations loss has been developed: 4.2% of ZZ→4μ events are corrected with an FSR selection purity of 95.6...

  12. Performance des jets et mesure de la section efficace de production de paires t tbar dans le canal tout hadronique auprès du détecteur ATLAS

    CERN Document Server

    Ghodbane, N

    In this report, we summarise our research program within the ATLAS collaboration between 2005-2012. We summarise our contribution to the integration of two of the Inner Detector sub-detectors, the SCT and the TRT. We describe also our contribution to the optimisation and tuning of the jet reconstruction in the harsh ATLAS environment. We compare the performances of these different algorithms. Finally, with the data collected at a centre of mass energy of 7 TeV, we extract the top-anti-top production cross section in the challenging all-hadronic decay channel.

  13. Search for excited leptons in the data of the H1 experiment at the HERA collider; Recherche de leptons excites dans les donnees de l'experience H1 aupres du collisionneur HERA

    Energy Technology Data Exchange (ETDEWEB)

    Delerue, N

    2002-05-01

    Composite models are one of the possible extensions of the Standard Model. One of their implications, at the energy in the reach of present particles accelerators, would be the excitation of leptons. This PhD. thesis describes the search for excited leptons with the H1 detector installed on the electron-proton collider HERA in Hamburg (Germany). The data used were accumulated between 1994 and 2000 and amount to an integrated luminosity of 120 pb{sup -1}. The analysis of 6 different topologies were done and cover all the branching ratios of deexcitation of excited electron and neutrino. The numbers of candidates found during those analysis is in agreement with the Standard Model expectations. This means that no evidence of excited leptons production was found at HERA. This result was translated in the form of exclusion limits on the coupling of excited leptons (f/{lambda}) depending on the mass of the excited lepton. For the first time at HERA we addressed the case were the natural decay width of the excited neutrino is wider than the experimental resolution. For the first time also, a study of the variation of limit depending on the ratio f'/f was carried out. This study lead to the setting of limits independent of this ratio. The limits obtained extend results previously obtained at HEA and also the results of direct searches at LEP. (author)

  14. Recherche de sgluons dans des états finals multitops avec le détecteur ATLAS auprès du LHC à $\\sqrt{s}$ = 8 TeV

    CERN Document Server

    Valery, Loïc; Calvet, Samuel

    Despite its experimental confirmations, the Standard Model, which describes both the elementary particles and three of the fundamental interactions, has some theoretical and experimental limitations. As a consequence of these limitations, a Physics not described in the context of the Standard Model could exist : the New Physics. This work focuses on the search for scalar gluons, commonly dubbed $sgluons$, predicted in various New Physics theories. A phenomenological study considers various final states (containing between two and four top quarks) and signatures (with one or two charged leptons) that could arise from sgluon production. The sensitivity of an ATLAS-like experiment to this signal is estimated and the results indicate that one of the most promising final states contains four top quarks in a signature with two charged leptons (electron or muon) of the same electric charge. The search for sgluons within the ATLAS experiment uses the previous results. Thus, it only investigates the 4-top topology i...

  15. Proposition d'attribution d'un contrat pour la fourniture d'aimants correcteurs a bobines decapolaires et octopolaires pour les aimants dipolaires supraconducteurs du LHC

    CERN Document Server

    1999-01-01

    Le présent document concerne l'attribution d'un contrat pour la fourniture de 616 aimants correcteurs à bobines décapolaires et octopolaires pour les aimants dipolaires supraconducteurs du LHC, avec une option pour fournir au maximum le même nombre d'aimants supplémentaires des mêmes types. A la suite d'une étude de marché (MS-2540/LHC/LHC) effectuée auprès de 39 entreprises dans treize Etats membres et deux entreprises au Japon, un appel d'offres (IT-2736/LHC/LHC) a été adressé le 24 juin 1999 à neuf entreprises dans six Etats membres et deux entreprises au Japon. A la date de clôture, le CERN avait reçu cinq offres. Il est demandé au Comité des finances d'approuver la négociation d'un contrat avec l'entreprise TESLA ENGINEERING (UK) pour la fourniture de 616 aimants correcteurs à bobines décapolaires et octopolaires pour les aimants dipolaires supraconducteurs à double ouverture du LHC, pour un montant total de 2 219 229 francs suisses, révisable pour les livraisons contractuelles pos...

  16. Le Parcours Étudiant du Festival Transamériques (FTA: une expérience de médiation culturelle marquante

    Directory of Open Access Journals (Sweden)

    Lucie

    2015-04-01

    Full Text Available Le but de cet article est de présenter les retombées éducatives du Parcours étudiant du FTA, consacré à la création contemporaine en théâtre et en danse au Québec. Une première enquête sur le terrain a été menée en 2010 auprès de 50 adolescents, suivie d’une autre, en 2014, afin de valider les résultats. La recherche nous révèle que l’évènement s’avère un rite de passage pour les jeunes ; il est source de découverte de soi tout autant qu’ouverture à l’altérité, et ce, tant au niveau de l’esthétique que sur les plans culturel et socio-politique.

  17. L’octroi de crédits aux femmes entrepreneuses libanaises par les banquiers : le cas du dispositif Kafalat

    Directory of Open Access Journals (Sweden)

    Inaya Wahidi

    2016-03-01

    Full Text Available L’accès au crédit bancaire sans garantie est quasi impossible au Liban, d’où le dispositif Kafalat qui représente une solution face à cette difficulté. Selon la littérature, l’entrepreneuriat des femmes souffre de discrimination par rapport aux hommes quant à l’octroi de crédits bancaires. Notre objectif est d’essayer de voir dans quelle mesure cette situation existe au Liban. L’étude exploratoire conduite par entretiens semi-directifs auprès des banquiers exclusivement fournit les premiers éléments sur le profil de ces femmes entrepreneuses libanaises et sur la discrimination éventuelle qui pourrait exister du fait de leur sexe pour l’obtention de crédits bancaires. Les résultats semblent montrer que les banquiers ne font pas de distinction entre les entrepreneurs hommes ou femmes, même si les entrepreneuses ont peut-être moins d’informations concernant les garanties offertes par le dispositif Kafalat et sont souvent soutenues par leur mari qui accepte une hypothèque comme garantie du crédit demandé par leur femme ou qui passe par leur femme pour obtenir le crédit nécessaire au développement de leur propre entreprise.

  18. Effets du fluor et du phosphogypse chez les organismes marins

    OpenAIRE

    Martin, J.L.; Le Guellec, Anne-marie; Cosson, R.

    1982-01-01

    Dans le cadre général des recherches visant à déterminer l'action des effluents industriels et plus précisément du fluor dans le cas de cette étude, le programme dont les résultats sont présentés avait pour but de déterminer les effets de cet élément sur les organismes marins. Trois aspects essentiels ont été envisagés : - Effets létaux du fluor ; - effets du fluor sur certaines fonctions éthologiques ; - bio-accumulation de l'élément par les organismes marins.

  19. Main: 1DU5 [RPSD[Archive

    Lifescience Database Archive (English)

    Full Text Available 1DU5 トウモロコシ Corn Zea mays L. Zeamatin Precursor. Name=Zlp; Zea Mays Molecule: Zeama...NNACPVFKKDEYCCVGSAANDCHPTNYSRYFKGQCPDAYSYPKDDATSTFTCPAGTNYKVVFCP corn_1DU5.jpg ...

  20. Cri du Chat syndrome

    Directory of Open Access Journals (Sweden)

    Cerruti Mainardi Paola

    2006-09-01

    Full Text Available Abstract The Cri du Chat syndrome (CdCS is a genetic disease resulting from a deletion of variable size occurring on the short arm of chromosome 5 (5p-. The incidence ranges from 1:15,000 to 1:50,000 live-born infants. The main clinical features are a high-pitched monochromatic cry, microcephaly, broad nasal bridge, epicanthal folds, micrognathia, abnormal dermatoglyphics, and severe psychomotor and mental retardation. Malformations, although not very frequent, may be present: cardiac, neurological and renal abnormalities, preauricular tags, syndactyly, hypospadias, and cryptorchidism. Molecular cytogenetic analysis has allowed a cytogenetic and phenotypic map of 5p to be defined, even if results from the studies reported up to now are not completely in agreement. Genotype-phenotype correlation studies showed a clinical and cytogenetic variability. The identification of phenotypic subsets associated with a specific size and type of deletion is of diagnostic and prognostic relevance. Specific growth and psychomotor development charts have been established. Two genes, Semaphorin F (SEMAF and δ-catenin (CTNND2, which have been mapped to the "critical regions", are potentially involved in cerebral development and their deletion may be associated with mental retardation in CdCS patients. Deletion of the telomerase reverse transcriptase (hTERT gene, localised to 5p15.33, could contribute to the phenotypic changes in CdCS. The critical regions were recently refined by using array comparative genomic hybridisation. The cat-like cry critical region was further narrowed using quantitative polymerase chain reaction (PCR and three candidate genes were characterised in this region. The diagnosis is based on typical clinical manifestations. Karyotype analysis and, in doubtful cases, FISH analysis will confirm the diagnosis. There is no specific therapy for CdCS but early rehabilitative and educational interventions improve the prognosis and considerable

  1. Gestion durable du paysage

    Directory of Open Access Journals (Sweden)

    Jean-David Gerber

    2009-03-01

    Full Text Available Le paysage est de plus en plus perçu comme une ressource. À ce titre, il est nécessaire de trouver des instruments juridiques, politiques ou économiques susceptibles de gérer cette « ressource-paysage » sur le long terme. Le gouvernement suisse a introduit récemment l’instrument des parcs naturels régionaux, organisés selon le modèle français, dans sa législation de protection de la nature et du paysage. Une mise en regard des nouveaux parcs avec des structures de gestion beaucoup plus anciennes, les bourgeoisies et les corporations, permet de mettre en évidence les forces et les faiblesses de chacun de ces instruments dans leur contribution à résoudre les rivalités d’usage entre acteurs utilisant ou influençant la ressource paysage. Cette comparaison permet de formuler des recommandations pratiques concernant la gestion de cette ressource.The landscape is increasingly perceived as a resource. For this reason, it is necessary to find legal, political and economic instruments that will succeed in managing this “resource landscape” in the long term. The Swiss government recently introduced the instrument of regional nature parks into the legislation governing nature and landscape preservation; the proposed parks are organized on the basis of the French model. The examination of the new parks from the perspective of much older management structures, i.e. the civic municipalities (bourgeoisies and corporations, makes it possible to demonstrate the strengths and weaknesses of each of these instruments in their contribution to the resolution of use rivalries between actors who use or influence the resource landscape. This comparison also enables the formulation of practical recommendations regarding the management of this resource.

  2. Les paradoxes du littoral Swahili

    Directory of Open Access Journals (Sweden)

    François Bart

    2008-10-01

    Full Text Available Le contact entre l'océan Indien occidental et le continent africain a forgé l'identité et l'originalité du littoral swahili. Cette interface, longue d'environ 2 000 kilomètres, du sud de la Somalie au nord du Mozambique, constitue un monde original où, au gré de traditions anciennes de circulation maritime et continentale se sont diffusées et mêlées des influences culturelles venues du continent africain, de la péninsule arabique et de la péninsule indienne. Le développement du continent, du littoral et des archipels s'inscrit dans une double logique de fragmentation et d'ouverture au monde. Dans cette vaste aire géographique, le rôle de relais des îles et des axes de pénétration continentale à partir des ports est essentiel.The identity and the original features of the Swahili seashore mainly proceed from the contact of African mainland and western indian Ocean. This coastal interface, stretching over 2 000 kilometres from southern Somalia to northern Mozambique, is characterized by ancient traditions of trade movements through maritime areas and mainland as well, which spread and mixed different cultural influences originating from Africa and both Arabic and Indian peninsulas. The development of this area is linked to both fragmentation and opening dynamics. In such a wide area, the relaying function of islands and continental corridors from main harbours is very important.

  3. Les conséquences du bouche-à-oreille électronique dans le secteur bancaire

    Directory of Open Access Journals (Sweden)

    Moez Ltifi

    2015-09-01

    Full Text Available Internet a changé la manière d’interagir entre l’entreprise et ses clients. L’étude de la manière dont le consommateur réagit face à l’adoption de nouvelles technologies d’information et de communication et en particulier les services bancaires en ligne, paraît une piste de recherche intéressante à approfondir. L’objectif de cette étude est de tester l’effet du bouche-à-oreille électronique sur l’image de marque de l’entreprise (banque, sur l’intention d’achat et sur l’attitude à l’égard de la banque. Une enquête a été conduite auprès d’un échantillon de 180 clients bancaires tunisiens. Les résultats révèlent que le bouche-à- oreille électronique influence positivement et significativement l’intention d’achat, l’image de marque et l’attitude à l’égard de la banque.

  4. Réflexion sur l’origine du processus de segmentation du marche du travail

    Directory of Open Access Journals (Sweden)

    Attia Nicole

    2006-01-01

    Full Text Available (francuski Ce travail propose une réflexion sur l'origine du processus de segmentation du marché du travail par rapport à l'entreprise. Se situe-t-elle au sein même de l'entreprise ou en amont, c'est à dire entre les entreprises? Cela revient à se demander si on peut avoir une approche microéconomique ou macroéconomique de la segmentation et, à s'interroger sur le rôle réel tenu par les firmes dans le processus. Déterminant pour la théorie, ce rôle est à repenser selon la réponse apportée à notre question.

  5. Radio-active pollution near natural uranium-graphite-gas reactors; La pollution radioactive aupres des piles uranium naturel - graphite - gaz

    Energy Technology Data Exchange (ETDEWEB)

    Chassany, J.; Pouthier, J.; Delmar, J. [Commissariat a l' Energie Atomique, Chusclan (France). Centre de Production de Plutonium de Marcoule

    1967-07-01

    The results of numerous evaluations of the contamination are given: - Reactors in operation during maintenance operations. - Reactors shut-down during typical repair operations (coolants, exchangers, interior of the vessel, etc. ) - Following incidents on the cooling circuit and can-rupture. They show that, except in particular cases, it is the activation products which dominate. Furthermore, after ten years operation, the points at which contamination liable to emit strong doses accumulates are very localized and the individual protective equipment has not had to be reinforced. (authors) [French] Les resultats de nombreuses evaluations de la contamination sont donnes: - Piles en marche pendant les operations d'entretien - Piles a l'arret au cours des chantiers caracteristiques (refrigerants, echangeurs, interieur du caisson, etc.) - A la suite d'incidents sur le circuit de refroidissement et de rupture de gaine. Ils montrent que, sauf cas particulier, ce sont essentiellement les produits d'activation qui dominent. Par ailleurs apres 10 ans de fonctionnement, les points d'accumulation de la contamination susceptibles de delivrer des debits de dose importants restent tres localises et les moyens de protection individuels utilises n'ont pas du etre renforces. (auteurs)

  6. L’orthographe du français. Ce qu’en pensent les formateurs et futurs formateurs

    Directory of Open Access Journals (Sweden)

    Moreau Marie-Louise

    2012-07-01

    Full Text Available Depuis 1900 au moins, la réforme de l’orthographe du français parait être en tout temps une question d’actualité. On ne peut être qu’impressionné par le nombre de commissions, projets, études, publications, pétitions, recommandations officielles... centrés sur cette thématique. L’époque actuelle semble même marquée par une certaine accélération, dont le point de départ pourrait être la publication au Journal officiel français, le 6 décembre 1990, des « rectifications orthographiques ». Toutes les publications scientifiques dédiées à cette question font état des difficultés que rencontrent les francophones dans l’écriture de leur langue. Beaucoup de ces travaux tentent de cerner les proportions respectives des pro- et des antiréformistes, analysent l’argumentaire des uns et des autres, essaient de déterminer sur quelles réformes les attentes pourraient s’accorder. C’est dans cette perspective que le présent travail s’inscrit, dans le contexte de la Belgique francophone. Dans cette communauté, en 1998, quatre circulaires ministérielles sont publiées à l’adresse des enseignants. Elles posent que les nouvelles graphies ont droit de cité dans l’enseignement, tout en mettant en avant un principe de tolérance : ni les nouvelles et ni les anciennes formes ne peuvent être considérées comme fautives. Ces circulaires n’ont apparemment suscité que des réactions assez molles. En septembre 2008, une nouvelle circulaire ministérielle (signée de quatre ministres se montre un peu plus incisive, invitant les enseignants, de tout niveau, à enseigner prioritairement les formes recommandées. La publication de ces circulaires s’est accompagnée de la diffusion, auprès de tous les enseignants, d’un dépliant, publié par le Service de la langue française, 7 Règles pour nous simplifier l’orthographe, qui synthétise les principales règles de la réforme. Remise alors sur le devant de la sc

  7. Son Excellence Madame Elisabeth Laurin Ambassadeur Représentant permanent de la France auprès de l’Office des Nations Unies et des autres organisations internationales en Suisse République française Son Excellence Monsieur Roberto Balzaretti Ambassadeur Directeur

    CERN Document Server

    AUTHOR|(CDS)2099575

    2016-01-01

    Son Excellence Madame Elisabeth Laurin Ambassadeur Représentant permanent de la France auprès de l’Office des Nations Unies et des autres organisations internationales en Suisse République française Son Excellence Monsieur Roberto Balzaretti Ambassadeur Directeur,

  8. Cri-du-chat syndrome

    NARCIS (Netherlands)

    Didden, H.C.M.; Curfs, L.M.G

    2013-01-01

    Cri-du-chat syndrome is a genetic disease resulting from a deletion occurring on the short arm of chromosome 5 (5p-). The incidence ranges from 1:15 000 to 1:50 000 live-born infants. Its main clinical features are a high-pitched monochromatic cry, microcephaly, broad nasal bridge, epicanthal folds,

  9. Review of Physics Results from the Tevatron: Searches for New Particles and Interactions

    Energy Technology Data Exchange (ETDEWEB)

    Toback, David [Texas A-M; ŽIvković, Lidija [Belgrade U.

    2015-02-17

    We present a summary of results for searches for new particles and interactions at the Fermilab Tevatron collider by the CDF and the D0 experiments. These include results from Run I as well as Run II for the time period up to July 2014. We focus on searches for supersymmetry, as well as other models of new physics such as new fermions and bosons, various models of excited fermions, leptoquarks, technicolor, hidden-valley model particles, long-lived particles, extra dimensions, dark matter particles, and signature-based searches.

  10. Combined effect of QCD resummation and QED radiative correction to W boson observables at the Tevatron.

    Science.gov (United States)

    Cao, Qing-Hong; Yuan, C P

    2004-07-23

    A precise determination of the W boson mass at the Fermilab Tevatron requires a theoretical calculation in which the effects of the initial-state multiple soft-gluon emission and the final-state photonic correction are simultaneously included. Here, we present such a calculation and discuss its prediction on the transverse mass distribution of the W boson and the transverse momentum distribution of its decay charged lepton, which are the most relevant observables for measuring the W boson mass at hadron colliders.

  11. First Measurements of Inclusive W and Z Cross Sections from Run II of the Tevatron Collider

    CERN Document Server

    Acosta, D; Akimoto, T; Albrow, M G; Ambrose, D; Amerio, S; Amidei, D; Anastassov, A; Anikeev, K; Annovi, A; Antos, J; Aoki, M; Apollinari, G; Arisawa, T; Arguin, J F; Artikov, A; Ashmanskas, W; Attal, A; Azfar, F; Azzi-Bacchetta, P; Bacchetta, N; Bachacou, H; Badgett, W; Barbaro-Galtieri, A; Barker, G J; Barnes, V E; Barnett, B A; Baroiant, S; Barone, M; Bauer, G; Bedeschi, F; Behari, S; Belforte, S; Bellettini, G; Bellinger, J; Benjamin, D; Beretvas, A; Bhatti, A A; Binkley, M; Bisello, D; Bishai, M; Blair, R E; Blocker, C; Bloom, K; Blumenfeld, B; Bocci, A; Bodek, A; Bölla, G; Bolshov, A; Booth, P S L; Bortoletto, D; Boudreau, J; Bourov, S; Bromberg, C; Brubaker, E; Budagov, Yu A; Budd, H S; Burkett, K; Busetto, G; Bussey, P; Byrum, K L; Cabrera, S; Calafiura, P; Campanelli, M; Campbell, M; Canepa, A; Casarsa, M; Carlsmith, D; Carron, S; Carosi, R; Cavalli-Sforza, M; Castro, A; Catastini, P; Cauz, D; Cerri, A; Cerri, C; Cerrito, L; Chapman, J; Chen, C; Chen, Y C; Chertok, M; Chiarelli, G; Chlachidze, G; Chlebana, F; Cho, I; Cho, K; Chokheli, D; Chu, M L; Chuang, S; Chung, J Y; Chung, W H; Chung, Y S; Ciobanu, C I; Ciocci, M A; Clark, A G; Clark, D; Coca, M; Connolly, A; Convery, M; Conway, J; Cooper, B; Cordelli, M; Cortiana, G; Cranshaw, J; Cuevas-Maestro, J; Culbertson, R; Currat, C; Cyr, D; Dagenhart, D; Da Ronco, S; D'Auria, S; De Barbaro, P; De Cecco, S; De Lentdecker, G; Dell'Agnello, S; Dell'Orso, Mauro; Demers, S; Demortier, L; Deninno, M; De Pedis, D; Derwent, P F; Dionisi, C; Dittmann, J R; Doksus, P; Dominguez, A; Donati, S; Donega, M; Donini, J; D'Onofrio, M; Dorigo, T; Drollinger, V; Ebina, K; Eddy, N; Ely, R; Erbacher, R; Erdmann, M; Errede, D; Errede, S; Eusebi, R; Fang, H C; Farrington, S; Fedorko, I; Feild, R G; Feindt, M; Fernández, J P; Ferretti, C; Field, R D; Fiori, I; Flanagan, G; Flaugher, B; Flores-Castillo, L R; Foland, A; Forrester, S; Foster, G W; Franklin, M; Freeman, J; Frisch, H; Fujii, Y; Furic, I; Gajjar, A; Gallas, A; Galyardt, J; Gallinaro, M; García-Sciveres, M; Garfinkel, A F; Gay, C; Gerberich, H; Gerdes, D W; Gerchtein, E; Giagu, S; Giannetti, P; Gibson, A; Gibson, K; Ginsburg, C; Giolo, K; Giordani, M; Giurgiu, G; Glagolev, V; Glenzinski, D; Gold, M; Goldschmidt, N; Goldstein, D; Goldstein, J; Gómez, G; Gómez-Ceballos, G; Goncharov, M; González, O; Gorelov, I; Goshaw, A T; Gotra, Yu; Goulianos, K; Gresele, A; Grosso-Pilcher, 4C; Günther, M; Guimarães da Costa, J; Haber, C; Hahn, K; Hahn, S R; Halkiadakis, E; Handler, R; Happacher, F; Hara, K; Hare, M; Harr, R F; Harris, R M; Hartmann, F; Hatakeyama, K; Hauser, J; Hays, C; Hayward, H; Heider, E; Heinemann, B; Heinrich, J; Hennecke, M; Herndon, M; Hill, C; Hirschbuehl, D; Höcker, A; Hoffman, K D; Holloway, A; Hou, S; Houlden, M A; Huffman, B T; Huang, Y; Hughes, R E; Huston, J; Ikado, K; Incandela, J R; Introzzi, G; Iori, M; Ishizawa, Y; Issever, C; Ivanov, A; Iwata, Y; Iyutin, B; James, E; Jang, D; Jarrell, J; Jeans, D; Jensen, H; Jeon, E J; Jones, M; Joo, K K; Jun, S; Junk, T R; Kamon, T; Kang, J; Karagoz-Unel, M; Karchin, P E; Kartal, S; Kato, Y; Kemp, Y; Kephart, R; Kerzel, U; Khotilovich, V; Kilminster, B; Kim, D H; Kim, H S; Kim, J E; Kim, M J; Kim, M S; Kim, S B; Kim, S H; Kim, T H; Kim, Y K; King, B T; Kirby, M; Kirsch, L; Klimenko, S; Knuteson, B; Ko, B R; Kobayashi, H; Koehn, P; Kong, D J; Kondo, K; Konigsberg, J; Kordas, K; Korn, A J; Korytov, A; Kotelnikov, K; Kotwal, A V; Kovalev, A; Kraus, J; Kravchenko, I; Kreymer, A; Kroll, J; Kruse, M; Krutelyov, V; Kuhlmann, S E; Kuznetsova, N; Laasanen, A T; Lai, S; Lami, S; Lammel, S; Lancaster, J; Lancaster, M; Lander, R; Lannon, K; Lath, A; Latino, G; Lauhakangas, R; Lazzizzera, I; Le, Y; Lecci, C; LeCompte, T; Lee, J; Lee, S W; Leonardo, N; Leone, S; Lewis, J D; Li, K; Lin, C; Lin, C S; Lindgren, M; Liss, T M; Litvintsev, D O; Liu, T; Liu, Y; Lockyer, N S; Loginov, A; Loreti, M; Loverre, P F; Lu, R S; Lucchesi, D; Lujan, P; Lukens, P; Lyons, L; Lys, J; Lysak, R; MacQueen, D; Madrak, R; Maeshima, K; Maksimovic, P; Malferrari, L; Manca, G; Marginean, R; Martin, M; Martin, A; Martin, V; Martínez, M; Maruyama, T; Matsunaga, H; Mattson, M; Mazzanti, P; McFarland, K S; McGivern, D; McIntyre, P M; McNamara, P; NcNulty, R; Menzemer, S; Menzione, A; Merkel, P; Mesropian, C; Messina, A; Miao, T; Miladinovic, N; Miller, L; Miller, R; Miller, J S; Miquel, R; Miscetti, S; Mitselmakher, G; Miyamoto, A; Miyazaki, Y; Moggi, N; Mohr, B; Moore, R; Morello, M; Moulik, T; Movilla-Fernández, P A; Mukherjee, A; Mulhearn, M; Müller, T; Mumford, R; Munar, A; Murat, P; Nachtman, J; Nahn, S; Nakamura, I; Nakano, I; Napier, A; Napora, R; Naumov, D V; Necula, V; Niell, F; Nielsen, J; Nelson, C; Nelson, T; Neu, C; Neubauer, M S; Newman-Holmes, C; Nicollerat, A S; Nigmanov, T; Nodulman, L; Norniella, O; Österberg, K; Ogawa, T; Oh, S H; Oh, Y D; Ohsugi, T; Okusawa, T; Oldeman, R G C; Orava, R; Orejudos, W; Pagliarone, C; Palmonari, F; Paoletti, R; Papadimitriou, V; Pashapour, S; Patrick, J; Pauletta, G; Paulini, M; Pauly, T; Paus, C; Pellett, D; Penzo, Aldo L; Phillips, T J; Piacentino, G; Piedra, J; Pitts, K T; Plager, C; Pompos, A; Pondrom, L; Pope, G; Poukhov, O; Prakoshyn, F; Pratt, T; Pronko, A; Proudfoot, J; Ptohos, F; Punzi, G; Rademacker, J; Rakitine, A; Rappoccio, S; Ratnikov, F; Ray, H; Reichold, A; Reisert, B; Rekovic, V; Renton, P B; Rescigno, M; Rimondi, F; Rinnert, K; Ristori, L; Robertson, W J; Robson, A; Rodrigo, T; Rolli, S; Rosenson, L; Roser, R; Rossin, R; Rott, C; Russ, J; Ruiz, A; Ryan, D; Saarikko, H; Safonov, A; Saint-Denis, R; Sakumoto, W K; Salamanna, G; Saltzberg, D; Sánchez, C; Sansoni, A; Santi, L; Sarkar, S; Sato, K; Savard, P; Savoy-Navarro, A; Schemitz, P; Schlabach, P; Schmidt, E E; Schmidt, M P; Schmitt, M; Scodellaro, L; Scribano, A; Scuri, F; Sedov, A; Seidel, S; Seiya, Y; Semeria, F; Sexton-Kennedy, L; Sfiligoi, I; Shapiro, M D; Shears, T G; Shepard, P F; Shimojima, M; Shochet, M; Shon, Y; Shreyber, I; Sidoti, A; Siegrist, J; Siket, M; Sill, A; Sinervo, P; Sissakian, A N; Skiba, A; Slaughter, A J; Sliwa, K; Smirnov, D; Smith, J R; Snider, F D; Snihur, R; Somalwar, S V; Spalding, J; Spezziga, M; Spiegel, L; Spinella, F; Spiropulu, M; Squillacioti, P; Stadie, H; Stefanini, A; Stelzer, B; Stelzer-Chilton, O; Strologas, J; Stuart, D; Sukhanov, A; Sumorok, K; Sun, H; Suzuki, T; Taffard, A C; Tafirout, R; Takach, S F; Takano, H; Takashima, R; Takeuchi, Y; Takikawa, K; Tanaka, M; Tanaka, R; Tanimoto, N; Tapprogge, Stefan; Tecchio, M; Teng, P K; Terashi, K; Tesarek, R J; Tether, S; Thom, J; Thompson, A S; Thomson, E; Tipton, P; Tiwari, V; Tkaczyk, S; Toback, D; Tollefson, K; Tomura, T; Tonelli, D; Tonnesmann, M; Torre, S; Torretta, D; Trischuk, W; Tseng, J; Tsuchiya, R; Tsuno, S; Tsybychev, D; Turini, N; Turner, M; Ukegawa, F; Unverhau, T; Uozumi, S; Usynin, D; Vacavant, L; Vaiciulis, A W; Varganov, A; Vataga, E; Vejcik, S; Velev, G V; Veramendi, G; Vickey, T; Vidal, R; Vila, I; Vilar, R; Volobuev, I P; Von der Mey, M; Wagner, R G; Wagner, R L; Wagner, W; Wallny, R; Walter, T; Yamashita, T; Yamamoto, K; Wan, Z; Wang, M J; Wang, S M; Warburton, A; Ward, B; Waschke, S; Waters, D; Watts, T; Weber, M; Wester, W C; Whitehouse, B; Wicklund, A B; Wicklund, E; Williams, H H; Wilson, P; Winer, B L; Wittich, P; Wolbers, S; Wolter, M; Worcester, M; Worm, S; Wright, T; Wu, X; Würthwein, F; Wyatt, A; Yagil, A; Yang, U K; Yao, W; Yeh, G P; Yi, K; Yoh, J; Yoon, P; Yorita, K; Yoshida, T; Yu, I; Yu, S; Yu, Z; Yun, J C; Zanello, L; Zanetti, A; Zaw, I; Zetti, F; Zhou, J; Zsenei, A; Zucchelli, S

    2004-01-01

    We report the first measurements of inclusive W and Z cross sections times leptonic branching ratios for p-pbar collisions at $\\sqrt{s} = 1.96$ TeV, based on their decays to electrons and muons. The data correspond to an integrated luminosity of 72 pb-1 recorded with the CDF detector at the Fermilab Tevatron. We test e-mu universality in W decays, and we measure the ratio of leptonic W and Z rates from which the leptonic branching fraction $B(W\\goto\\ell\

  12. Reshimming of Tevatron Dipoles; A Process-Quality and Lessons-Learned Perspective

    CERN Document Server

    Blowers, James N; Harding, David J; John, Carson; Robotham, William

    2005-01-01

    Over the last two years corrections have been made for the skew quadrupole moment in 530 of the 774 installed dipoles in the Tevatron. This process of modifying the magnets in situ has inherent risk of degrading the performance of the superconducting accelerator. In order to manage the risk, as well as to ensure the corrections were done consistently, formal quality tools were used to plan and verify the work. The quality tools used to define the process and for quality control are discussed, along with highlights of lessons learned.

  13. Factorization breaking in single-diffractive dijet production at the Tevatron

    Science.gov (United States)

    Klasen, Michael

    2010-10-01

    We perform a NLO QCD analysis of single-diffractive dijet production in proton-antiproton collisions. By comparing the ratio of single- and non-diffractive cross sections to data from the Tevatron, the rapidity-gap survival probability is determined as a function of the momentum fraction of the parton in the antiproton. Assuming Regge factorization, this probability can be interpreted as a suppression factor for the diffractive structure function measured in deep-inelastic scattering at HERA. In contrast to the observations for photoproduction, the suppression factor in proton-antiproton collisions depends on the momentum fraction of the parton in the Pomeron even at NLO.

  14. Factorization breaking in single-diffractive dijet production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Klasen, Michael, E-mail: klasen@lpsc.in2p3.f [Laboratoire de Physique Subatomique et de Cosmologie, Universite Joseph Fourier / CNRS-IN2P3 / INPG, 53 Avenue des Martyrs, F-38026 Grenoble (France)

    2010-10-15

    We perform a NLO QCD analysis of single-diffractive dijet production in proton-antiproton collisions. By comparing the ratio of single- and non-diffractive cross sections to data from the Tevatron, the rapidity-gap survival probability is determined as a function of the momentum fraction of the parton in the antiproton. Assuming Regge factorization, this probability can be interpreted as a suppression factor for the diffractive structure function measured in deep-inelastic scattering at HERA. In contrast to the observations for photoproduction, the suppression factor in proton-antiproton collisions depends on the momentum fraction of the parton in the Pomeron even at NLO.

  15. NLO QCD analysis of single-diffractive dijet production at the Tevatron

    Science.gov (United States)

    Klasen, M.

    We present the first NLO QCD analysis of single-diffractive dijet production in proton-antiproton collisions. By comparing the ratio of single- and non-diffractive cross sections to data from the Tevatron, the rapidity-gap survival probability is determined as a function of the momentum fraction of the parton in the antiproton. Assuming Regge factorization, this probability can be interpreted as a suppression factor for the diffractive structure function measured in deep-inelastic scattering at HERA. In contrast to the observations for photoproduction, the suppression factor in proton-antiproton collisions depends on the momentum fraction of the parton in the Pomeron even at NLO.

  16. Factorization breaking in single-diffractive dijet production at the Tevatron

    CERN Document Server

    Klasen, M

    2010-01-01

    We perform a NLO QCD analysis of single-diffractive dijet production in proton-antiproton collisions. By comparing the ratio of single- and non-diffractive cross sections to data from the Tevatron, the rapidity-gap survival probability is determined as a function of the momentum fraction of the parton in the antiproton. Assuming Regge factorization, this probability can be interpreted as a suppression factor for the diffractive structure function measured in deep-inelastic scattering at HERA. In contrast to the observations for photoproduction, the suppression factor in proton-antiproton collisions depends on the momentum fraction of the parton in the Pomeron even at NLO.

  17. NLO QCD analysis of single-diffractive dijet production at the Tevatron

    CERN Document Server

    Klasen, M

    2010-01-01

    We present the first NLO QCD analysis of single-diffractive dijet production in proton-antiproton collisions. By comparing the ratio of single- and non-diffractive cross sections to data from the Tevatron, the rapidity-gap survival probability is determined as a function of the momentum fraction of the parton in the antiproton. Assuming Regge factorization, this probability can be interpreted as a suppression factor for the diffractive structure function measured in deep-inelastic scattering at HERA. In contrast to the observations for photoproduction, the suppression factor in proton-antiproton collisions depends on the momentum fraction of the parton in the Pomeron even at NLO.

  18. Fragmentation contributions to J/ψ production at the Tevatron and the LHC.

    Science.gov (United States)

    Bodwin, Geoffrey T; Chung, Hee Sok; Kim, U-Rae; Lee, Jungil

    2014-07-11

    We compute leading-power fragmentation corrections to J/ψ production at the Tevatron and the LHC. We find that, when these corrections are combined with perturbative corrections through next-to-leading order in the strong coupling constant α(s), we obtain a good fit to high-p(T) cross section data from the CDF and CMS Collaborations. The fitted long-distance matrix elements lead to predictions of near-zero J/ψ polarization in the helicity frame at large p(T).

  19. Longitudinal bunch monitoring at the Fermilab Tevatron and Main Injector synchrotrons

    CERN Document Server

    Thurman-Keup, R; Blokland, W; Crisp, J; Eddy, N; Fellenz, B; Flora, R; Hahn, A; Hansen, S; Kiper, T; Para, A; Pordes, S; Tollestrup, A V

    2011-01-01

    The measurement of the longitudinal behavior of the accelerated particle beams at Fermilab is crucial to the optimization and control of the beam and the maximizing of the integrated luminosity for the particle physics experiments. Longitudinal measurements in the Tevatron and Main Injector synchrotrons are based on the analysis of signals from resistive wall current monitors. This article describes the signal processing performed by a 2 GHz-bandwidth oscilloscope together with a computer running a LabVIEW program which calculates the longitudinal beam parameters.

  20. Measurements of the masses, lifetimes and decay modes of hadrons at Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Dorigo, Mirco; /Trieste U. /INFN, Trieste

    2010-05-01

    The Tevatron provides 1.96 TeV p{bar p} collisions and allows for collection of rich b-hadron samples to the two experiments CDF and D0. The study of heavy flavor properties represents a fruitful opportunity to investigate the flavor sector of the Standard Model (SM) and to look for hints of New Physics (NP). Here we report the first measurement of polarization amplitudes in B{sub s}{sup 0} charmless decays, world leading results on b-hadron lifetimes, and measurements of several other properties of b-hadrons.

  1. Probing top anomalous couplings at the Tevatron and the Large Hadron Collider

    Indian Academy of Sciences (India)

    Debajyoti Choudhury; Pratishruti Saha

    2011-12-01

    Chromomagnetic and chromoelectric dipole interactions of the top quark are studied in a model-independent framework. Limits are set on the scale of new physics that might lead to such contributions using latest Tevatron measurements of the $t\\bar{t}$ cross-section. It is demonstrated that the invariant mass distribution is a sensitive probe. Prospects at the LHC are examined. It is shown that, for unitarized amplitudes, an increase in the LHC energy is of little importance, while the accumulation of luminosity plays a crucial role.

  2. Non-inclusive searches for squarks and gluinos at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Biscarat, Catherine; /Lyon, IPN

    2007-11-01

    Recent results from the CDF and D0 Collaborations on searches for squarks and gluinos at the Run II of the Fermilab Tevatron collider are presented. This review covers searches for final states involving specific mass hierarchies. The analyzed datasets correspond to an integrated luminosity of 300-1000 pb{sup -1} collected from proton anti-proton collisions at a center-of-mass energy of 1.96 TeV. No significant deviations from the Standard Model expectations are observed and limits on parameters of supersymmetry are set in generic MSSM and in specific mSUGRA scenarios.

  3. Collective flow in (anti)proton-proton collision at Tevatron and LHC

    CERN Document Server

    Pierog, Tanguy; Karpenko, Iurii; Werner, Klaus

    2010-01-01

    Collective flow as a consequence of hydrodynamical evolution in heavy ion collisions is intensively studied by theorists and experimentalists to understand the behavior of hot quark matter. Due to their large mass, heavy ions suffer collective effects even at low (SPS) or intermediate energies (RHIC). In case of light systems such as (anti)proton-proton interactions, collective effects was not expected. Within a global model such as EPOS, where light and heavy systems are treated using the same physics, it appears that Tevatron data are better described if a flow is introduced. Then the extrapolation to LHC can easily be done and we can compare to first data from ATLAS experiment.

  4. Soft multiple parton interactions as seen in multiplicity distributions at Tevatron and LHC

    CERN Document Server

    Dremin, I M

    2011-01-01

    We analyse the multiplicity distributions of charged particles at Tevatron (p\\bar p) and LHC (pp) energies in the framework of the independent pair parton interactions (IPPI) model. It is shown that the number of soft pair parton interactions (and therefore the density of the partonic medium) is large and increases with energy. The mean multiplicity at each parton interaction grows also with energy. This growth depends on the width of the rapidity window. The similar conclusions are obtained in the multiladder exchange model (QGSM).

  5. Search for chargino and neutralino at Run II of the Tevatron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Canepa, Anadi [Purdue Univ., West Lafayette, IN (United States)

    2006-08-01

    In this dissertation we present a search for the associated production of charginos and neutralinos, the supersymmetric partners of the Standard Model bosons. We analyze a data sample representing 745 pb-1 of integrated luminosity collected by the CDF experiment at the p$\\bar{p}$ Tevatron collider. We compare the Standard Model predictions with the observed data selecting events with three leptons and missing transverse energy. Finding no excess, we combine the results of our search with similar analyses carried out at CDF and set an upper limit on the chargino mass in SUSY scenarios.

  6. First measurement of the W-boson mass in run II of the Tevatron.

    Science.gov (United States)

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Cavalli-Sforza, M; Cerri, A; Cerrito, L; Chang, S H; Chen, Y C; Chertok, M; Chiarelli, G; Chlachidze, G; Chlebana, F; Cho, I; Cho, K; Chokheli, D; Chou, J P; Choudalakis, G; Chuang, S H; Chung, K; Chung, W H; Chung, Y S; Cilijak, M; Ciobanu, C I; Ciocci, M A; Clark, A; Clark, D; Coca, M; Compostella, G; Convery, M E; Conway, J; Cooper, B; Copic, K; Cordelli, M; Cortiana, G; Crescioli, F; Almenar, C Cuenca; Cuevas, J; Culbertson, R; Cully, J C; Daronco, S; Datta, M; D'Auria, S; Davies, T; Dagenhart, D; de Barbaro, P; De Cecco, S; Deisher, A; De Lentdecker, G; De Lorenzo, G; Dell'orso, M; Delli Paoli, F; Demortier, L; Deng, J; Deninno, M; De Pedis, D; Derwent, P F; Di Giovanni, G P; Dionisi, C; Di Ruzza, B; Dittmann, J R; D'Onofrio, M; Dörr, C; Donati, S; Dong, P; Donini, J; Dorigo, T; Dube, S; Efron, J; Erbacher, R; Errede, D; Errede, S; Eusebi, R; Fang, H C; Farrington, S; Fedorko, I; Fedorko, W T; Feild, R G; Feindt, M; Fernandez, J P; Field, R; Flanagan, G; Forrest, R; Forrester, S; Franklin, M; Freeman, J C; Furic, I; Gallinaro, M; Galyardt, J; Garcia, J E; Garberson, F; Garfinkel, A F; Gay, C; Gerberich, H; Gerdes, D; Giagu, S; Giannetti, P; Gibson, K; Gimmell, J L; Ginsburg, C; Giokaris, N; Giordani, M; Giromini, P; Giunta, M; Giurgiu, G; Glagolev, V; Glenzinski, D; Gold, M; Goldschmidt, N; Goldstein, J; Golossanov, A; Gomez, G; Gomez-Ceballos, G; Goncharov, M; González, O; Gorelov, I; Goshaw, A T; Goulianos, K; Gresele, A; Grinstein, S; Grosso-Pilcher, C; Grundler, U; da Costa, J Guimaraes; Gunay-Unalan, Z; Haber, C; Hahn, K; Hahn, S R; Halkiadakis, E; Hamilton, A; Han, B-Y; Han, J Y; Handler, R; Happacher, F; Hara, K; Hare, D; Hare, M; Harper, S; Harr, R F; Harris, R M; Hartz, M; Hatakeyama, K; Hauser, J; Hays, C; Heck, M; Heijboer, A; Heinemann, B; Heinrich, J; Henderson, C; Herndon, M; Heuser, J; Hidas, D; Hill, C S; Hirschbuehl, D; Hocker, A; Holloway, A; Hou, S; Houlden, M; Hsu, S-C; Huffman, B T; Hughes, R E; Husemann, U; Huston, J; Incandela, J; Introzzi, G; 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Lungu, G; Lyons, L; Lys, J; Lysak, R; Lytken, E; Mack, P; Macqueen, D; Madrak, R; Maeshima, K; Makhoul, K; Maki, T; Maksimovic, P; Malde, S; Malik, S; Manca, G; Manousakis, A; Margaroli, F; Marginean, R; Marino, C; Marino, C P; Martin, A; Martin, M; Martin, V; Martínez, M; Martínez-Ballarín, R; Maruyama, T; Mastrandrea, P; Masubuchi, T; Matsunaga, H; Mattson, M E; Mazini, R; Mazzanti, P; McFarland, K S; McIntyre, P; McNulty, R; Mehta, A; Mehtala, P; Menzemer, S; Menzione, A; Merkel, P; Mesropian, C; Messina, A; Miao, T; Miladinovic, N; Miles, J; Miller, R; Mills, C; Milnik, M; Mitra, A; Mitselmakher, G; Miyamoto, A; Moed, S; Moggi, N; Mohr, B; Moon, C S; Moore, R; Morello, M; Fernandez, P Movilla; Mülmenstädt, J; Mukherjee, A; Muller, Th; Mumford, R; Murat, P; Mussini, M; Nachtman, J; Nagano, A; Naganoma, J; Nakamura, K; Nakano, I; Napier, A; Necula, V; Neu, C; Neubauer, M S; Nielsen, J; Nodulman, L; Norniella, O; Nurse, E; Oh, S H; Oh, Y D; Oksuzian, I; Okusawa, T; Oldeman, R; Orava, R; Osterberg, K; Pagliarone, C; Palencia, E; Papadimitriou, V; Papaikonomou, A; Paramonov, A A; Parks, B; Pashapour, S; Patrick, J; Pauletta, G; Paulini, M; Paus, C; Pellett, D E; Penzo, A; Phillips, T J; Piacentino, G; Piedra, J; Pinera, L; Pitts, K; Plager, C; Pondrom, L; Portell, X; Poukhov, O; Pounder, N; Prakoshyn, F; Pronko, A; Proudfoot, J; Ptohos, F; Punzi, G; Pursley, J; Rademacker, J; Rahaman, A; Ramakrishnan, V; Ranjan, N; Redondo, I; Reisert, B; Rekovic, V; Renton, P; Rescigno, M; Richter, S; Rimondi, F; Ristori, L; Robson, A; Rodrigo, T; Rogers, E; Rolli, S; Roser, R; Rossi, M; Rossin, R; Roy, P; Ruiz, A; Russ, J; Rusu, V; Saarikko, H; Safonov, A; Sakumoto, W K; Salamanna, G; Saltó, O; Santi, L; Sarkar, S; Sartori, L; Sato, K; Savard, P; Savoy-Navarro, A; Scheidle, T; Schlabach, P; Schmidt, E E; Schmidt, M P; Schmitt, M; Schwarz, T; Scodellaro, L; Scott, A L; Scribano, A; Scuri, F; Sedov, A; Seidel, S; Seiya, Y; Semenov, A; Sexton-Kennedy, L; Sfyrla, A; Shalhout, S Z; Shapiro, M D; Shears, T; Shepard, P F; Sherman, D; Shimojima, M; Shochet, M; Shon, Y; Shreyber, I; Sidoti, A; Sinervo, P; Sisakyan, A; Slaughter, A J; Slaunwhite, J; Sliwa, K; Smith, J R; Snider, F D; Snihur, R; Soderberg, M; Soha, A; Somalwar, S; Sorin, V; Spalding, J; Spinella, F; Spreitzer, T; Squillacioti, P; Stanitzki, M; Staveris-Polykalas, A; Denis, R St; Stelzer, B; Stelzer-Chilton, O; Stentz, D; Strologas, J; Stuart, D; Suh, J S; Sukhanov, A; Sun, H; Suslov, I; Suzuki, T; Taffard, A; Takashima, R; Takeuchi, Y; Tanaka, R; Tecchio, M; Teng, P K; Terashi, K; Thom, J; Thompson, A S; Thomson, E; Tipton, P; Tiwari, V; Tkaczyk, S; Toback, D; Tokar, S; Tollefson, K; Tomura, T; Tonelli, D; Torre, S; Torretta, D; Tourneur, S; Trischuk, W; Tsuno, S; Tu, Y; Turini, N; Ukegawa, F; Uozumi, S; Vallecorsa, S; van Remortel, N; Varganov, A; Vataga, E; Vazquez, F; Velev, G; Vellidis, C; Veramendi, G; Veszpremi, V; Vidal, M; Vidal, R; Vila, I; Vilar, R; Vine, T; Vogel, M; Vollrath, I; Volobouev, I; Volpi, G; Würthwein, F; Wagner, P; Wagner, R G; Wagner, R L; Wagner, J; Wagner, W; Wallny, R; Wang, S M; Warburton, A; Waters, D; Weinberger, M; Wester, W C; Whitehouse, B; Whiteson, D; Wicklund, A B; Wicklund, E; Williams, G; Williams, H H; Wilson, P; Winer, B L; Wittich, P; Wolbers, S; Wolfe, C; Wright, T; Wu, X; Wynne, S M; Yagil, A; Yamamoto, K; Yamaoka, J; Yamashita, T; Yang, C; Yang, U K; Yang, Y C; Yao, W M; Yeh, G P; Yoh, J; Yorita, K; Yoshida, T; Yu, G B; Yu, I; Yu, S S; Yun, J C; Zanello, L; Zanetti, A; Zaw, I; Zhang, X; Zhou, J; Zucchelli, S

    2007-10-12

    We present a measurement of the W-boson mass using 200 pb{-1} of data collected in pp[over ] collisions at sqrt[s]=1.96 TeV by the CDF II detector at run II of the Fermilab Tevatron. With a sample of 63 964 W-->enu candidates and 51 128 W-->munu candidates, we measure M_{W}=80 413+/-34{stat}+/-34{syst}=80,413+/-48 MeV/c;{2}. This is the most precise single measurement of the W-boson mass to date.

  7. B(s) Mixing, Delta Gamma(s) and CP Violation at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Di Giovanni, Gian Piero; /Paris U., VI-VII

    2008-05-01

    The authors discuss the results from the Tevatron experiments on mixing and CP violation in the B{sub s}{sup 0}-{bar B}{sub s}{sup 0} system, with particular emphasis to the updated measurements of the decay-width difference {Delta}{Lambda}{sub s} and the first measurement of the CP-violating phase {beta}{sub s} using flavor tagging information. They also briefly review the charge asymmetry measurements in semileptonic B{sub s}{sup 0} decays and in B{sup {+-}} {yields} J/{psi}K{sup {+-}} decays.

  8. Jet Substructure at the Tevatron and LHC: New results, new tools, new benchmarks

    CERN Document Server

    Altheimer, A; Asquith, L; Brooijmans, G; Butterworth, J; Campanelli, M; Chapleau, B; Cholakian, A E; Chou, J P; Dasgupta, M; Davison, A; Dolen, J; Ellis, S D; Essig, R; Fan, J J; Field, R; Fregoso, A; Gallicchio, J; Gershtein, Y; Gomes, A; Haas, A; Halkiadakis, E; Halyo, V; Hoeche, S; Hook, A; Hornig, A; Huang, P; Izaguirre, E; Jankowiak, M; Kribs, G; Krohn, D; Larkoski, A J; Lath, A; Lee, C; Lee, S J; Loch, P; Maksimovic, P; Martinez, M; Miller, D W; Plehn, T; Prokofiev, K; Rahmat, R; Rappoccio, S; Safonov, A; Salam, G P; Schumann, S; Schwartz, M D; Schwartzman, A; Seymour, M; Shao, J; Sinervo, P; Son, M; Soper, D E; Spannowsky, M; Stewart, I W; Strassler, M; Strauss, E; Takeuchi, M; Thaler, J; Thomas, S; Tweedie, B; Vasquez Sierra, R; Vermilion, C K; Villaplana, M; Vos, M; Wacker, J; Walker, D; Walsh, J R; Wang, L-T; Wilbur, S; Yavin, I; Zhu, W

    2012-01-01

    In this report we review recent theoretical progress and the latest experimental results in jet substructure from the Tevatron and the LHC. We review the status of and outlook for calculation and simulation tools for studying jet substructure. Following up on the report of the Boost 2010 workshop, we present a new set of benchmark comparisons of substructure techniques, focusing on the set of variables and grooming methods that are collectively known as "top taggers". To facilitate further exploration, we have attempted to collect, harmonise, and publish software implementations of these techniques.

  9. Model Independent Searches for New Physics at the Fermilab Tevatron Collider

    CERN Document Server

    Piper, Joel

    2009-01-01

    The standard model is a successful but limited theory. There is significant theoretical motivation to believe that new physics may appear at the energy scale of a few TeV, the lower end of which is currently probed by the Fermilab Tevatron Collider. The methods used to search for physics beyond the standard model in a model independent way and the results of these searches based on 1.0 fb-1 of data collected with the D0 detector and 2.0 fb^-1 at the CDF detector are presented.

  10. The Tevatron Higgs exclusion limits and theoretical uncertainties: a critical appraisal

    CERN Document Server

    Baglio, J; Ferrag, S; Godbole, R M

    2011-01-01

    We examine the exclusion limits set by the CDF and D0 experiments on the Standard Model Higgs boson mass from their searches at the Tevatron in the light of large theoretical uncertainties on the signal and background cross sections. We show that when these uncertainties are consistently taken into account, the sensitivity of the experiments becomes significantly lower and the currently excluded mass range $M_H=158$-175 GeV would be entirely reopened. The necessary luminosity required to recover the current sensitivity is found to be a factor of two higher than the present one.

  11. First measurement of the W boson mass in run II of the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Aaltonen, T.; Abulencia, A.; /Helsinki Inst. of Phys.; Adelman, J.; /Illinois U., Urbana; Affolder, Anthony Allen; /Chicago U., EFI; Akimoto, T.; /UC, Santa Barbara; Albrow, Michael G.; /Tsukuba U.; Amerio, S.; /Fermilab; Amidei, Dante E.; /Padua U.; Anastassov, A.; /Michigan U.; Anikeev, K.; /Rutgers U., Piscataway; Annovi, A.; /Fermilab /Frascati /Comenius U.

    2007-07-01

    We present a measurement of the W boson mass using 200 pb{sup -1} of data collected in p{bar p} collisions at {radical}s = 1.96 TeV by the CDF II detector at Run II of the Fermilab Tevatron. With a sample of 63964 W {yields} ev candidates and 51128 W W {yields} {mu}v candidates, we measure M{sub W} = (80413 {+-} 34{sub stat} {+-}34{sub syst} = 80413 {+-} 48) MeV/c{sup 2}. This is the most precise single measurement of the W boson mass to date.

  12. La « faillite » du ciblage monétaire en Tunisie ?

    Directory of Open Access Journals (Sweden)

    Rima Lajnaf

    2014-09-01

    Full Text Available Les monétaristes ont montré que l’accélération de la masse monétaire ne ferait qu’attiser l’inflation. Leur idée a gagné en influence auprès des banques centrales, les incitant dans les années soixante-dix à s’efforcer de mieux maîtriser l’inflation en utilisant les agrégats monétaires comme les variables de leurs objectifs intermédiaires. Cependant, même si l’utilisation des cibles monétaires est répandue dans le monde entier, il n’existe pas de consensus sur la causalité entre la monnaie et les prix. Ce problème a fait l’objet d’un débat très animé entre les économistes surtout durant les trois dernières décennies caractérisées par l’innovation financière. La stratégie de ciblage de l’agrégat monétaire n’est efficace que si ce dernier, considéré comme une cible intermédiaire, possède des propriétés satisfaisantes en termes de stabilité, de contrôlabilité et du contenu en information. Dans ce papier, nous allons étudier l’efficacité de la politique d’ancrage monétaire en Tunisie en analysant les propriétés de l’agrégat M3. Les résultats montrent que le choix de cet agrégat comme un objectif intermédiaire ne semble pas être justifié.

  13. Preparation of the ATLAS experiment in the LHC proton collider, performances of the electromagnetic calorimeter and its potentialities for the top quark; Preparation de l'experience ATLAS aupres du futur grand collisionneur de protons LHC: performances du calorimetre electromagnetique et potentiels pour la physique du quark top

    Energy Technology Data Exchange (ETDEWEB)

    Hubaut, F

    2007-03-15

    ATLAS is the biggest and the more complex detector ever built, it will operate on the LHC and is the outcome of a huge international collaboration of 2000 physicists. This document reviews the theoretical and experimental achievements of one of them, his collaboration spread over 7 years and has followed 2 axis. First, the design, construction and test of the electromagnetic calorimeter of ATLAS and secondly, the development of analysis strategies in the physics of the top quark. The expected important production of top quarks in LHC will allow an accurate measurement of the properties of this particle and in the same way will provide new testing areas for the standard model. The top quark, being extremely massive, might play a significant role in the mechanism of electro-weak symmetry breaking. This document is organized into 5 chapters: 1) ATLAS detector, performance and progress, 2) the optimization of the energy measurement with the electromagnetic calorimeter, 3) the performance of the electromagnetic calorimeter, 4) the physics of the top quark, and 5) the potentialities of ATLAS in the top quark sector. This document presented before an academic board will allow its author to manage research works and particularly to tutor thesis students. (A.C.)

  14. Performance du calorimètre à argon liquide et recherche du boson de Higgs dans son canal de désintégration $H\\to ZZ^{(*)} \\to 4\\ell$ avec l'expérience ATLAS auprès du LHC.

    CERN Document Server

    Tiouchichine, Elodie

    The work presented in this thesis within the ATLAS collaboration was performed in the context of the discovery of a new particle at the LHC in the search for the Standard Model Higgs boson. My contribution to the Higgs boson search is focused in the $H \\to ZZ^* \\to 4 \\ell$ channel at different level, from the data taking to the physics analysis. After a theoretical introduction, the LHC and the ATLAS detector are presented as well as their performance during the 2011 and 2012 runs. A particular consideration is given to the liquid argon calorimeters and to the data quality assessment of this system. The validation of the data recorded during non-nominal high voltage conditions is presented. This study allowed to recover 2\\% of the data collected available for physics analyses. This has a direct impact on the $H \\to ZZ^* \\to 4 \\ell$ channel were the number of signal events expected is very low. In order to optimize the acceptance of the four electrons decay channel, novel electron reconstruction algorithms wer...

  15. LES GITES PLOMBO-ZINCIFERES DU DISTRICT MINIER DU KOUDIAT SIDU AUSUD DU KEF EN TUNISIE

    Directory of Open Access Journals (Sweden)

    Ivan Jurković

    1992-12-01

    Full Text Available Les auteurs ont dćcrit l:i stratigiaphie. I.i tectonique, le corps de minerals, la paragenese et la genese dcs gttes Koudiat Sidri situ&s environ 20 km au sud de la ville du Kef en Tunisie.

  16. Multiple Parton Interactions in p$bar{p}$ Collisions in D0 Experiment at the Tevatron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Golovanov, Georgy [Joint Inst. for Nuclear Research (JINR), Dubna (Russia)

    2016-01-01

    The thesis is devoted to the study of processes with multiple parton interactions (MPI) in a ppbar collision collected by D0 detector at the Fermilab Tevatron collider at sqrt(s) = 1.96 TeV. The study includes measurements of MPI event fraction and effective cross section, a process-independent parameter related to the effective interaction region inside the nucleon. The measurements are done using events with a photon and three hadronic jets in the final state. The measured effective cross section is used to estimate background from MPI for WH production at the Tevatron energy

  17. R-parity violating decays of the Top-Quark and the Top-Squark at the Tevatron

    CERN Document Server

    De Campos, F; Éboli, Oscar J P; Magro, M B; Navarro, L; Porod, Werner; Restrepo, D A; Valle, José W F

    1999-01-01

    We study unconventional decays of the top-quark and the top-squark in the framework of SUSY models with broken R-parity. The model under study is the MSSM with an additional bilinear term that breaks R-parity. In this model the top-squark behaves similar to a third generation leptoquark. We demonstrate that existing Tevatron data on the top give rise to restrictions on the SUSY parameter space. In particular, we focus on scenarios where the tau-neutrino mass is smaller than 1 eV. We give an exclusion plot derived from the leptoquark searches at Tevatron.

  18. Dynamique narrative du texte, du film et de la musique

    OpenAIRE

    Wildgen, Wolfgang

    2015-01-01

    La narrativité est foncièrement liée à la dynamique des événements et des actions représentés, et elle dépend du champ pragmatique narrateur/récepteur, c’est-à-dire du discours narratif. Cette dynamique demande une théorisation adéquate, par exemple au sein de la théorie des systèmes dynamiques ou de l’analyse vectorielle, et elle se manifeste dans des modalités différentes. Nous présentons des exemples d’analyse dans la modalité linguistique (récit oral spontané, conte populaire), dans la mo...

  19. Le parcours migratoire de jeunes ruraux du bled du kif

    Directory of Open Access Journals (Sweden)

    Khalid Mouna

    2015-06-01

    Full Text Available Cet article analyse le parcours migratoire des jeunes ruraux originaires des zones de production du cannabis, jeunes qui cherchent à briser les chaînes de soumission et d’humiliation vécues au quotidien. Pour les jeunes concernés par notre étude, la migration constitue un moyen de s’intégrer dans des réseaux transnationaux et ainsi d’entamer une carrière de beznass (commerçant du cannabis. Ce parcours « initiatique » permet à ces jeunes de revenir au bled avec de nouvelles idées, des moyens accrus, et de jouer un rôle actif dans l’économie locale – qui reste pour eux focalisée sur la production de cannabis, cette dernière restant néanmoins officiellement interdite.

  20. Probing the TC2 model via Production of Top Quark Pairs at Tevatron and LHC

    Institute of Scientific and Technical Information of China (English)

    GU Qin-Zhong; YANG Hua; WANG Xue-Lei

    2007-01-01

    The topcolour-assisted technicolour (TC2) model is an interesting dynamical theory among the various new physics models. We calculate the total t(t) cross section and the relative correction of the TC2 model to the cross section at Tevatron Run Ⅱ and LHC. At the Tevatron Run Ⅱ, the cross section predicted by the standard model (SM) is consistent with the experimental data, and in most parameter spaces of the TC2 model, the relative correction of the TC2 model to the cross section is too small to be detectable. We find that the t(t) cross section is more sensitive to the parameters of the TC2 model at the LHC and the relative correction of the TC2 model to the cross section is over 10% in general. Such a value of the relative correction should be large enough to be detectable at the LHC. Therefore, it is promising to find the clue of the TC2 model via the t(t) production at the LHC.

  1. The Reach of the Fermilab Tevatron and CERN LHC for Gaugino Mediated SUSY Breaking Models

    CERN Document Server

    Baer, Howard W; Krupovnickas, T; Tata, Xerxes; Baer, Howard; Belyaev, Alexander; Krupovnickas, Tadas; Tata, Xerxes

    2002-01-01

    In supersymmetric models with gaugino mediated SUSY breaking (inoMSB), it is assumed that SUSY breaking on a hidden brane is communicated to the visible brane via gauge superfields which propagate in the bulk. This leads to GUT models where the common gaugino mass $m_{1/2}$ is the only soft SUSY breaking term to receive contributions at tree level. To obtain a viable phenomenology, it is assumed that the gaugino mass is induced at some scale $M_c$ beyond the GUT scale, and that additional renormalization group running takes place between $M_c$ and $M_{GUT}$ as in a SUSY GUT. We assume an SU(5) SUSY GUT above the GUT scale, and compute the SUSY particle spectrum expected in models with inoMSB. We use the Monte Carlo program ISAJET to simulate signals within the inoMSB model, and compute the SUSY reach including cuts and triggers approriate to Fermilab Tevatron and CERN LHC experiments. We find no reach for SUSY by the Tevatron collider in the trilepton channel. %either with or without %identified tau leptons. ...

  2. Reach of the Fermilab Tevatron and CERN LHC for gaugino mediated SUSY breaking models

    CERN Document Server

    Baer, Howard W; Krupovnickas, T; Tata, Xerxes; 10.1103/PhysRevD.65.075024

    2002-01-01

    In supersymmetric models with gaugino mediated SUSY breaking (gMSB), it is assumed that SUSY breaking on a hidden brane is communicated to the visible brane via gauge superfields which propagate in the bulk. This leads to GUT models where the common gaugino mass m/sub 1/2/ is the only soft SUSY breaking term to receive contributions at the tree level. To obtain a viable phenomenology, it is assumed that the gaugino mass is induced at some scale M/sub c/ beyond the GUT scale, and that additional renormalization group running takes place between M/sub c/ and M/sub GUT/ as in a SUSY GUT. We assume an SU(5) SUSY GUT above the GUT scale, and compute the SUSY particle spectrum expected in models with gMSB. We use the Monte Carlo program ISAJET to simulate signals within the gMSB model, and compute the SUSY reach including cuts and triggers appropriate to Fermilab Tevatron and CERN LHC experiments. We find no reach for SUSY by the Tevatron collider in the trilepton channel. At the CERN LHC, values of m/sub 1/2/=1000...

  3. LHC Predictions from a Tevatron Anomaly in the Top Quark Forward-Backward Asymmetry

    Energy Technology Data Exchange (ETDEWEB)

    Bai, Yang; Hewett, JoAnne L.; Kaplan, Jared; Rizzo, Thomas G.; /SLAC

    2011-08-12

    We examine the implications of the recent CDF measurement of the top-quark forward-backward asymmetry, focusing on a scenario with a new color octet vector boson at 1-3 TeV. We study several models, as well as a general effective field theory, and determine the parameter space which provides the best simultaneous fit to the CDF asymmetry, the Tevatron top pair production cross section, and the exclusion regions from LHC dijet resonance and contact interaction searches. Flavor constraints on these models are more subtle and less severe than the literature indicates. We find a large region of allowed parameter space at high axigluon mass and a smaller region at low mass; we match the latter to an SU(3){sub 1} x SU(3){sub 2}/SU(3){sub c} coset model with a heavy vector-like fermion. Our scenario produces discoverable effects at the LHC with only 1-2 inverse femtobarns of luminosity at 7-8 TeV. Lastly, we point out that a Tevatron measurement of the b-quark forward-backward asymmetry would be very helpful in characterizing the physics underlying the top-quark asymmetry.

  4. Non-perturbative QCD Effects and the Top Mass at the Tevatron

    CERN Document Server

    Wicke, Daniel

    2008-01-01

    The modelling of non-perturbative effects is an important part of modern collider physics simulations. In hadron collisions there is some indication that the modelling of the interactions of the beam remnants, the underlying event, may require non-trivial colour reconnection effects to be present. We recently introduced a universally applicable toy model of such reconnections, based on hadronising strings. This model, which has one free parameter, has been implemented in the Pythia event generator. We then considered several parameter sets (`tunes'), constrained by fits to Tevatron minimum-bias data, and determined the sensitivity of a simplified top mass analysis to these effects, in exclusive semi-leptonic top events at the Tevatron. A first attempt at isolating the genuine non-perturbative effects gave an estimate of order +-0.5GeV from non-perturbative uncertainties. The results presented here are an update to the original study and include recent bug fixes of Pythia that influenced the tunings investigat...

  5. Polarized J/psi production from B mesons at the Tevatron

    CERN Document Server

    Krey, U

    2003-01-01

    In the framework of NRQCD and parton model, we estimate in detail,the production cross section for polarized J/psi from B meson decays. In order to contrast with data, we also take into account additional J/psi production due to decay of excited charmonium states. We calculate the helicity parameter, alpha, and as an application, we study our results for the Tevatron. This is in contrast to the earlier studies which were performed for prompt J/psi production from p pbar collisions. Our estimates are, for J/psi from B decays, alpha_{J/psi} = -0.04 +- 0.06 and for B decays to psi', alpha_{psi'}= -0.03 +- 0.07. These results have been evaluated in the J/psi transverse momentum interval, 10 GeV < k_T < 30 GeV. In the limit of the color singlet model, alpha shows a direct dependence on the Peterson parameter, thereby reflecting the dynamics of the b quark hadronization. With Run II of the Tevatron, it is expected that the fits for alpha will improve by about a factor of 50, leading to better limits on the ma...

  6. L’Harmonie du monde

    Directory of Open Access Journals (Sweden)

    Martine Clouzot

    2003-11-01

    Full Text Available La Bourgogne est particulièrement bien présente et représentée dans l’exposition sur la musique et ses représentations au Moyen Âge organisée par Isabelle Marchesin (université de Poitiers, Christine Laloue (conservatrice du Patrimoine au Musée et Martine Clouzot (université de Bourgogne, au Musée de la Musique à Paris du 26 mars au 27 juin 2004. En Côte-d’Or, à Dijon, la Bibliothèque municipale a donné son accord officiel pour le prêt de la Bible d’Etienne Harding, les Moralia in Job et u...

  7. L'energie du moustique

    CERN Document Server

    Augereau, J F

    2002-01-01

    ENSEMBLE DE QUATRE ARTICLES - LARGE HADRON COLLIDER: Le dernier accelerateur de particules du CERN, le LEP, produisait des faisceaux d'electrons de 100 GeV chacun. Le LHC, qui accelere des faisceaux de protons, leur communiquera une energie de 7 TeV chacun. Une energie a la fois colossale et derisoire. Un TeV represente a peu pres l'energie cinetique d'un moustique (1/2 page).

  8. Prairie du Chien: A Historical Study,

    Science.gov (United States)

    1976-10-01

    Naudouwessee with whom this governor made peace and introduced trade and commerce among the whole nation. His son the successor told me that some of the...Nicholas Perrot, French Commandant of the West, with a party of couriers du bois and voyageurs descended the Wisconsin River and erected Fort St...number of traders and voyageurs settled at Prairie du Chien. Thomas Anderson who settled at Prairie du Chien in 1800 described the conditions on his

  9. Search for supersymmetric Higgs bosons in the D0 experiment at the Tevatron; Recherche de bosons de Higgs supersymetriques au Tevatron dans l'experience D0

    Energy Technology Data Exchange (ETDEWEB)

    Michaut, M

    2006-09-15

    A search for the neutral Higgs bosons of the minimal supersymmetric extension of the standard model is performed in the 3 or 4 jets channels, pp-bar {yields} {phi}({yields} bb-bar)b(b-bar) with {phi} = h, H or A. For this purpose, the data collected with the D0 detector from 2002 to 2006 at the Tevatron hadronic collider with a center of mass energy of 1.96 TeV are analyzed. A complete study of the triggering is first done. The triggering conditions are optimized in order to keep the more signal fraction possible. Furthermore, a method is developed to predict the triggering efficiencies on our signal and backgrounds using only the data. Then an analysis method that allows the prediction of our background without the help of simulations is studied. No excess in events is observed in the data sample analyzed, corresponding to an integrated luminosity of 0.9 fb{sup -1}, so limits are set in the minimal supersymmetric extension of the standard model. At 95% confidence level, the following limits are found: tan({beta}) < 46 - 121 for m{sub {phi}} equals 100 - 170 GeV. (author)

  10. Genetics Home Reference: cri-du-chat syndrome

    Science.gov (United States)

    ... Health Conditions cri-du-chat syndrome cri-du-chat syndrome Enable Javascript to view the expand/collapse ... PDF Open All Close All Description Cri-du-chat (cat's cry) syndrome, also known as 5p- (5p ...

  11. Au fil du temps (1976 ou la loi du seuil

    Directory of Open Access Journals (Sweden)

    Isabelle Singer

    2010-04-01

    Full Text Available Ayant choisi de vivre dans un camion, les héros d’Au fil du temps (film de Wim Wenders de 1976 font du seuil une expérience particulière. Celle de la rupture avec toute idée de foyer et celle du refus d’appartenance à la terre natale, cette terre allemande traversée par une frontière le long de laquelle ils vont voyager, et qui les renvoie à chaque instant aux traumatismes de l’Histoire. Sur le pare-brise du camion, l’extérieur (campagnes indifférenciées, villes à l’abandon… et l’intérieur se superposent. Au fil du temps questionne le paysage : il s’agit d’en décoller un à un les mythes qui le recouvrent. L’image alors n’est plus surface mais volume à traverser, à lacérer et découvrir ce qui est tissé dans le paysage. La démarche de Wenders est alors proche de celle d’un de ses contemporains : Anselm Kiefer. Le paysage allemand provoque le rejet parce qu’il y a là toujours plus que le visible : des strates et des strates de culpabilité que le mythe - et c’est sa fonction - a recouvert. Et qu’il s’agira ici, de soulever. Le choix du nomadisme, c’est celui d’un état de l’humanité antérieur à l’idée de patrie. Et c’est aussi celui de la solitude, comme prix à payer à ce refus d’appartenance et à cette mise à jour des mythes. L’appartenance à la terre allemande et à son Histoire est profondément problématique parce que les pères sont fondamentalement coupables. On se reconnaîtra alors des pères de substitution : des pères de cinéma (Nicholas Ray ou Fritz Lang. Et l’on substituera l’Histoire du cinéma à l’Histoire. Bruno est réparateur ambulant de projecteurs et Au fil du temps dressera, au gré de ses pérégrinations, un état des lieux du cinéma allemand des années soixante-dix : déliquescent, colonisé par les images hollywoodiennes. Il faut que cela change : état du cinéma ; état des protagonistes solitaires en quête d’une identit

  12. Coil Creep and Skew-Quadrupole Field Components in the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Annala, G.; Harding, D.J.; Syphers, M.J.; /Fermilab

    2011-07-11

    During the start-up of Run II of the Tevatron Collider program, several issues surfaced which were not present, or not seen as detrimental, during Run I. These included the repeated deterioration of the closed orbit requiring orbit smoothing every two weeks or so, the inability to correct the closed orbit to desired positions due to various correctors running at maximum limits, regions of systematically strong vertical dipole corrections, and the identification of very strong coupling between the two transverse degrees-of-freedom. It became apparent that many of the problems being experienced operationally were connected to a deterioration of the main dipole magnet alignment, and remedial actions were undertaken. However, the alignment alone was not enough to explain the corrector strengths required to handle transverse coupling. With one exception, strong coupling had generally not been an issue in the Tevatron during Run I. Based on experience with the Main Ring, the Tevatron was designed with a very strong skew quadrupole circuit to compensate any quadrupole alignment and skew quadrupole field errors that might present themselves. The circuit was composed of 48 correctors placed evenly throughout the arcs, 8 per sector, evenly placed in every other cell. Other smaller circuits were installed but not initially needed or commissioned. These smaller circuits were composed of individual skew quadrupole correctors on either side of the long straight sections. These circuits were tuned by first bringing the horizontal and vertical tunes near each other. The skew quadrupoles were then adjusted to minimize tune split, usually to less than 0.003. Initially, the main skew quad circuit (designated T:SQ) could accomplish this global decoupling with only 4% of its possible current, and the smaller circuits were not required at all. The start-up of Run Ib was complicated by what was later discovered to be a rolled triplet quadrupole magnet in one of the Interaction Regions

  13. Dépendance économique aux produits forestiers non ligneux : cas des ménages riverains des forêts de Boulon et de Koflandé, au Sud-Ouest du Burkina Faso

    DEFF Research Database (Denmark)

    Ouédraogo, M; Ouédraogo, D; Thiombiano, T;

    2013-01-01

    Cette étude a pour objectif d’évaluer la dépendance économique des ménages riverains des forêts de Boulon et de Koflandé aux produits forestiers non ligneux (PFNL) et d’identifier les déterminants de cette dépendance. Des enquêtes ont été menées auprès de 583 ménages de 14 villages riverains de ces...... forêts. Les résultats montrent que le revenu moyen annuel par ménage est de 846 800 F CFA avec une contribution de 60% du revenu des cultures et 12% du revenu d’élevage. Les PFNL procurent en moyenne 72 479 F CFA par ménage et par an à près de 93% des ménages enquêtés. La dépendance économique des...... ménages aux PFNL est estimée à 12%. Elle diminue avec le revenu, traduisant une plus grande dépendance des ménages pauvres aux PFNL. Par ailleurs, les hommes sont économiquement moins dépendants des PFNL que les femmes. Les autres déterminants de la dépendance aux PFNL sont le statut d’autochtone, la...

  14. Du e-portfolio à l’analyse du produit et du processus de conception du projet personnel de l’étudiant

    OpenAIRE

    Huguette Albernhe-Giordan; Stéphanie Mailles-Viard Metz

    2008-01-01

    [Français] L’étude vise à évaluer l’effet de la conception d’un e-portfolio par des étudiants sur la méthode de construction de leur projet professionnel personnalisé. Le e-portfolio doit permettre à l’étudiant, guidé par un processus de conception –soutenu par une réflexion ergonomique– de développer de manière autonome son projet. Une étude a été menée sur une période de deux années auprès d’un public d’étudiants en institut universitaire de technologie, spécialisation informatique. Les rés...

  15. Search for the Higgs-Boson with the CDF experiment at Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Hennecke, Martin [Univ. of Karlsruhe (Germany)

    2005-06-10

    A search for a low-mass SM Higgs-Boson in the channel WH → lvb$\\bar{b}$ has been performed using neural networks. The data were taken by the CDF experiment at the p-$\\bar{p}$ collider Tevatron from 2000-2003, corresponding to in integrated luminosity of Lint = 162 pb-1 at a CMS-energy of √s = 1.96 TeV. 95% confidence level upper limits are set on σ × BR, the product of the production cross section times the Branching ratio, as a function of the Higgs boson mass. Cross sections above 8 pb are excluded for six different Higgs masses between 110 GeV/c2 and 150 GeV/c2. The required integrated luminosities for a 95% C.L. exclusion, 3σ evidence and 5σ discovery are calculated.

  16. Asymmetries in W^+/- and Z^0/gamma^* production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Halkiadakis, E.; /Rochester U.

    2004-12-01

    The authors describe a measurement of the charge asymmetry of electrons from W{sup {+-}} boson decays using p{bar p} {yields} W {yields} e{nu} events. They also present a measurement of the forward-backward charge asymmetry of electron-positron pairs resulting from the process p{bar p} {yields} Z{sup 0}/{gamma}* {yields} e{sup +}e{sup -}, from which they extract the Z{sup 0}-quark and Z{sup 0}-electron coupling constants and measure the sensitivity of the CDF experiment to these couplings. These analyses use integrated luminosities of 170 pb{sup -1} and 72 pb{sup -1}, respectively, of data collected by the CDF Run II detector at the Fermilab Tevatron.

  17. Search for production of single top quarks via flavor-changing neutral currents at the Tevatron

    CERN Document Server

    Abazov, V M; Abolins, M; Acharya, B S; Adams, M; Adams, T; Aguiló, E; Ahn, S H; Ahsan, M; Alexeev, G D; Alkhazov, G; Alton, A; Alverson, G; Alves, G A; Anastasoaie, M; Ancu, L S; Andeen, T; Anderson, S; Andrieu, B; Anzelc, M S; Arnoud, Y; Arov, M; Askew, A; Assis-Jesus, A C S; Atramentov, O; Autermann, C; Avila, C; Ay, C; Badaud, F; Baden, A; Bagby, L; Baldin, B; Bandurin, D V; Banerjee, P; Banerjee, S; Barberis, E; Barfuss, A F; Bargassa, P; Baringer, P; Barnes, C; Barreto, J; Bartlett, J F; Bassler, U; Bauer, D; Beale, S; Bean, A; Begalli, M; Begel, M; Belanger-Champagne, C; Bellantoni, L; Bellavance, A; Benítez, J A; Beri, S B; Bernardi, G; Bernhard, R; Berntzon, L; Bertram, I; Besançon, M; Beuselinck, R; Bezzubov, V A; Bhat, P C; Bhatnagar, V; Binder, M; Biscarat, C; Blackler, I; Blazey, G; Blekman, F; Blessing, S; Bloch, D; Bloom, K; Boline, D; Bolton, T A; Boos, E E; Borissov, G; Bos, K; Bose, T; Brandt, A; Brock, R; Brooijmans, G; Bross, A; Brown, D; Buchanan, N J; Buchholz, D; Bunichev, V; Burdin, S; Burke, S; Burnett, T H; Busato, E; Buszello, C P; Butler, J M; Böhnlein, A; Bühler, M; Büscher, V; Calfayan, P; Calvet, S; Cammin, J; Caron, S; Carvalho, W; Casey, B C K; Cason, N M; Castilla-Valdez, H; Chakrabarti, S; Chakraborty, D; Chan, K; Chan, K M; Chandra, A; Charles, F; Cheu, E; Chevallier, F; Cho, D K; Choi, S; Choudhary, B; Christofek, L; Christoudias, T; Claes, D; Clement, B; Clément, C; Coadou, Y; Cooke, M; Cooper, W E; Corcoran, M; Couderc, F; Cousinou, M C; Cox, B; Crepe-Renaudin, S; Cutts, D; Da Motta, H; Das, A; Davies, B; Davies, G; De Jong, S J; De La Cruz-Burelo, E; De Oliveira Martins, C; De, K; Degenhardt, J D; Demarteau, M; Demina, R; Denisov, D; Denisov, S P; Desai, S; Diehl, H T; Diesburg, M; Doidge, M; Dominguez, A; Dong, H; Dudko, L V; Duflot, L; Dugad, S R; Duggan, D; Duperrin, A; Dyer, J; Dyshkant, A; Déliot, F; Eads, M; Edmunds, D; Ellison, J; Elvira, V D; Enari, Y; Eno, S; Ermolov, P; Evans, H; Evdokimov, A; Evdokimov, V N; Ferapontov, A V; Ferbel, T; Fiedler, F; Filthaut, F; Fisher, W; Fisk, H E; Ford, M; Fortner, M; Fox, H; Fu, S; Fuess, S; Gadfort, T; Galea, C F; Gallas, E; Galyaev, E; García, C; García-Bellido, A; Gavrilov, V; Gay, P; Geist, W; Gelé, D; Gerber, C E; Gershtein, Yu; Gillberg, D; Ginther, G; Gollub, N; Goussiou, A; Grannis, P D; Greenlee, H; Greenwood, Z D; Gregores, E M; Grenier, G; Gris, P; Grivaz, J F; Grohsjean, A; Grünendahl, S; Grünewald, M W; Guo, F; Guo, J; Gutíerrez, G; Gutíerrez, P; Gómez, B; Haas, A; Hadley, N J; Haefner, P; Hagopian, S; Haley, J; Hall, I; Hall, R E; Han, L; Hanagaki, K; Hansson, P; Harder, K; Harel, A; Harrington, R; Hauptman, J M; Hauser, R; Hays, J; Hebbeker, T; Hedin, D; Hegeman, J G; Heinmiller, J M; Heinson, A P; Heintz, U; Hensel, C; Herner, K; Hesketh, G; Hildreth, M D; Hirosky, R; Hobbs, J D; Hoeneisen, B; Hoeth, H; Hohlfeld, M; Hong, S J; Hooper, R; Houben, P; Hu, Y; Hubacek, Z; Hynek, V; Iashvili, I; Illingworth, R; Ito, A S; Jabeen, S; Jaffré, M; Jain, S; Jakobs, K; Jarvis, C; Jenkins, A; Jesik, R; Johns, K; Johnson, C; Johnson, M; Jonckheere, A; Jonsson, P; Juste, A; Kahn, S; Kajfasz, E; Kalinin, A M; Kalk, J M; Kalk, J R; Kappler, S; Karmanov, D; Kasper, J; Kasper, P; Katsanos, I; Kau, D; Kaur, R; Kehoe, R; Kermiche, S; Khalatyan, N; Khanov, A; Kharchilava, A I; Kharzheev, Yu M; Khatidze, D; Kim, H; Kim, T J; Kirby, M H; Klima, B; Kohli, J M; Konrath, J P; Kopal, M; Korablev, V M; Kotcher, J; Kothari, B; Koubarovsky, A; Kozelov, A V; Krop, D; Kryemadhi, A; Kumar, A; Kunori, S; Kupco, A; Kurca, T; Kvita, J; Käfer, D; Kühl, T; Lam, D; Lammers, S; Landsberg, G L; Lazoflores, J; Lebrun, P; Lee, W M; Leflat, A; Lehner, F; Lesne, V; Lewis, P; Li, J; Li, L; Li, Q Z; Lietti, S M; Lima, J G R; Lincoln, D; Linnemann, J; Lipaev, V V; Lipton, R; Liu, Z; Lobo, L; Lobodenko, A; Lokajícek, M; Lounis, A; Love, P; Lubatti, H J; Lynker, M; Lyon, A L; Lévêque, J; Cwiok, M; Maciel, A K A; Madaras, R J; Magass, C; Magerkurth, A; Makovec, N; Mal, P K; Malbouisson, H B; Malik, S; Malyshev, V L; Mao, H S; Maravin, Y; Martin, B; McCarthy, R; Melnitchouk, A; Mendes, A; Mendoza, L; Mercadante, P G; Merkin, M; Merritt, K W; Meyer, A; Meyer, J; Michaut, M; Miettinen, H; Millet, T; Mitrevski, J; Molina, J; Mommsen, R K; Mondal, N K; Monk, J; Moore, R W; Moulik, T; Muanza, G S; Mulders, M; Mulhearn, M; Mundal, O; Mundim, L; Mättig, P; Nagy, E; Naimuddin, M; Narain, M; Naumann, N A; Neal, H A; Negret, J P; Neustroev, P; Nilsen, H; Nomerotski, A; Novaes, S F; Nunnemann, T; Nöding, C; O'Dell, V; O'Neil, D C; Obrant, G; Ochando, C; Oguri, V; Oliveira, N; Onoprienko, D; Oshima, N; Osta, J; Otec, R; Oteroy-Garzon, G J; Owen, M; Padley, P; Pangilinan, M; Parashar, N; Park, S J; Park, S K; Parsons, J; Partridge, R; Parua, N; Patwa, A; Pawloski, G; Perea, P M; Perfilov, M; Peters, K; Peters, Y; Petroff, P; Petteni, M; Piegaia, R; Piper, J; Pleier, M A; Podesta-Lerma, P L M; Podstavkov, V M; Pogorelov, Y; Pol, M E; Pompos, A; Pope, B G; Popov, A V; Potter, C; Prado da Silva, W L; Prosper, H B; Protopopescu, S D; Qian, J; Quadt, A; Quinn, B; Rangel, M S; Rani, K J; Ranjan, K; Ratoff, P N; Renkel, P; Reucroft, S; Rijssenbeek, M; Ripp-Baudot, I; Rizatdinova, F K; Robinson, S; Rodrigues, R F; Royon, C; Rubinov, P; Ruchti, R; Wang, M H L; Sajot, G; Sanders, M P; Santoro, A F S; Savage, G; Sawyer, L; Scanlon, T; Schaile, A D; Schamberger, R D; Scheglov, Y; Schellman, H; Schieferdecker, P; Schmitt, C; Schwanenberger, C; Schwartzman, A; Schwienhorst, R; Sekaric, J; Sen-Gupta, S; Severini, H; Shabalina, E; Shamim, M; Shary, V; Shchukin, A A; Shivpuri, R K; Shpakov, D; Siccardi, V; Sidwell, R A; Simák, V; Sirotenko, V I; Skubic, P L; Slattery, P F; Smirnov, D; Smith, R P; Snow, G R; Snow, J; Snyder, S; Sonnenschein, L; Sopczak, A; Sosebee, M; Soustruznik, K; Souza, M; Spurlock, B; Stark, J; Steele, J; Stolin, V; Stone, A; Stoyanova, D A; Strandberg, J; Strandberg, S; Strang, M A; Strauss, M; Strom, D; Strovink, M; Ströhmer, R; Stutte, L; Sumowidagdo, S; Svoisky, P; Sznajder, A; Sánchez-Hernández, A; Söldner-Rembold, S; Talby, M; Tamburello, P; Taylor, W; Telford, P; Temple, J; Tiller, B; Tissandier, F; Titov, M; Tokmenin, V V; Tomoto, M; Toole, T; Torchiani, I; Trefzger, T; Trincaz-Duvoid, S; Tsybychev, D; Tuchming, B; Tully, C; Tuts, P M; Unalan, R; Uvarov, L; Uvarov, S; Uzunyan, S; Vachon, B; Van Kooten, R; Van Leeuwen, W M; Van den Berg, P J; Varelas, N; Varnes, E W; Vartapetian, A H; Vasilyev, I A; Vaupel, M; Verdier, P; Vertogradov, L S; Verzocchi, M; Villeneuve-Séguier, F; Vint, P; Vlimant, J R; Von Törne, E; Voutilainen, M; Vreeswijk, M; Wahl, H D; Wang, L; Warchol, J; Watts, G; Wayne, M; Weber, G; Weber, M; Weerts, H; Wenger, A; Wermes, N; Wetstein, M; White, A; Wicke, D; Wilson, G W; Wimpenny, S J; Wobisch, M; Wood, D R; Wyatt, T R; Xie, Y; Yacoob, S; Yamada, R; Yan, M; Yasuda, T; Yatsunenko, Y A; Yip, K; Yoo, H D; Youn, S W; Yu, C; Yu, J; Yurkewicz, A; Zatserklyaniy, A; Zeitnitz, C; Zhang, D; Zhao, T; Zhou, B; Zhu, J; Zielinski, M; Zieminska, D; Zieminski, A; Zutshi, V; Zverev, E G; de Jong, P; van Eijk, B; Åsman, B

    2007-01-01

    We search for the production of single top quarks via flavor-changing neutral current couplings of a gluon to the top quark and a charm (c) or up (u) quark. We analyze 230 pb^{-1} of lepton+jets data from \\ppbar collisions at a center of mass energy of 1.96 TeV collected by the D0 detector at the Fermilab Tevatron Collider. We observe no significant deviation from standard model predictions, and hence set upper limits on anomalous coupling parameters \\kappa^c_g/\\Lambda and \\kappa^u_g/\\Lambda, where the \\kappa_g define the strength of the tcg and tug couplings, and \\Lambda defines the scale of new physics. The limits at 95% C.L. are: \\kappa^c_g/\\Lambda < 0.15 TeV^{-1} and \\kappa^u_g/\\Lambda < 0.037 TeV^{-1}.

  18. A search for double-charged Higgs bosons at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Baraoiant, Sasha [Univ. of California, Davis, CA (United States)

    2006-01-01

    We search for the pair production of doubly charged Higgs particles followed by the lepton-flavor violating decay of each Higgs into electron-and-tau and muon-and-tau pairs using 350 pb-1 of data collected by the CDF II experiment at the Fermilab Tevatron. Separate searches investigate cases where three or four final state leptons are detected, and the limits for each exclusive decay mode reflect the combined results of both searches. Assuming the H$±±\\atop{L}$ decays exclusively into like sign electron-and-tau pairs, we set a lower limit on its mass of 114 GeV/c2 at the 95 % confidence level. In the case of exclusive muon-and-tau decays, we set a lower mass limit of 112 GeV/c2 also at the 95% confidence level.

  19. A Study for Doubly-Charged Higgs Boson at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Baroiant, Sasha [Univ. of California, Davis, CA (United States)

    2006-01-01

    We search for the pair production of doubly charged Higgs particles followed by the lepton-flavor violating decay of each Higgs into electron-and-tau and muonand- tau pairs using 350 pb-1 of data collected by the CDF II experiment at the Fermilab Tevatron. Separate searches investigate cases where three or four finalstate leptons are detected, and the limits for each exclusive decay mode reflect the combined results of both searches. Assuming the H$±±\\atop{L}$ decays exclusively into likesign electron-and-tau pairs, we set a lower limit on its mass of 114 GeV/c2 at the 95 % confidence level. In the case of exclusive muon-and-tau decays, we set a lower mass limit of 112 GeV/c2 also at the 95% confidence level.

  20. Search for Neutral Higgs Bosons in Events with Multiple Bottom Quarks at the Tevatron

    CERN Document Server

    Aaltonen, T; Abbott, B; Acharya, B.S; Adams, M; Adams, T; Alexeev, G.D; Alkhazov, G; Alton, A; Alvarez Gonzalez, B; Alverson, G; Amerio, S; Amidei, D; Anastassov, A; Annovi, A; Antos, J; Apollinari, G; Appel, J.A; Arisawa, T; Artikov, A; Asaadi, J; Ashmanskas, W; Askew, A; Atkins, S; Auerbach, B; Augsten, K; Aurisano, A; Avila, C; Azfar, F; Badaud, F; Badgett, W; Bae, T; Bagby, L; Baldin, B; Bandurin, D.V; Banerjee, S; Barbaro-Galtieri, A; Barberis, E; Baringer, P; Barnes, V.E; Barnett, B.A; Barria, P; Bartlett, J.F; Bartos, P; Bassler, U; Bauce, M; Bazterra, V; Bean, A; Bedeschi, F; Begalli, M; Behari, S; Bellantoni, L; Bellettini, G; Bellinger, J; Benjamin, D; Beretvas, A; Beri, S.B; Bernardi, G; Bernhard, R; Bertram, I; Besancon, M; Beuselinck, R; Bhat, P.C; Bhatia, S; Bhatnagar, V; Bhatti, A; Bisello, D; Bizjak, I; Bland, K.R; Blazey, G; Blessing, S; Bloom, K; Blumenfeld, B; Bocci, A; Bodek, A; Boehnlein, A; Boline, D; Boos, E.E; Borissov, G; Bortoletto, D; Bose, T; Boudreau, J; Boveia, A; Brandt, A; Brandt, O; Brigliadori, L; Brock, R; Bromberg, C; Bross, A; Brown, D; Brown, J; Brucken, E; Budagov, J; Bu, X.B; Budd, H.S; Buehler, M; Buescher, V; Bunichev, V; Burdin, S; Burkett, K; Busetto, G; Bussey, P; Buszello, C.P; Buzatu, A; Calamba, A; Calancha, C; Camacho-Perez, E; Camarda, S; Campanelli, M; Campbell, M; Canelli, F; Carls, B; Carlsmith, D; Carosi, R; Carrillo, S; Carron, S; Casal, B; Casarsa, M; Casey, B.C.K; Castilla-Valdez, H; Castro, A; Catastini, P; Caughron, S; Cauz, D; Cavaliere, V; Cavalli-Sforza, M; Cerri, A; Cerrito, L; Chakrabarti, S; Chakraborty, D; Chan, K.M; Chandra, A; Chapon, E; Chen, G; Chen, Y.C; Chertok, M; Chevalier-Thery, S; Chiarelli, G; Chlachidze, G; Chlebana, F; Cho, D.K; Cho, K; Cho, S.W; Choi, S; Chokheli, D; Choudhary, B; Chung, W.H; Chung, Y.S; Cihangir, S; Ciocci, M.A; Claes, D; Clark, A; Clarke, C; Clutter, J; Compostella, G; Convery, M.E; Conway, J; Cooke, M; Cooper, W.E; Corbo, M; Corcoran, M; Cordelli, M; Couderc, F; Cousinou, M.C; Cox, C.A; Cox, D.J; Crescioli, F; Croc, A; Cuevas, J; Culbertson, R; Cutts, D; Dagenhart, D; d'Ascenzo, N; Das, A; Datta, M; Davies, G; de Barbaro, P; de Jong, S., J; De La Cruz-Burelo, E; Deliot, F; Dell'Orso, M; Demina, R; Demortier, L; Deninno, M; Denisov, D; Denisov, S.P; d'Errico, M; Desai, S; Deterre, C; DeVaughan, K; Devoto, F; Di Canto, A; Di Ruzza, B; Diehl, H.T; Diesburg, M; Ding, P.F; Dittmann, J.R; Dominguez, A; Donati, S; Dong, P; D'Onofrio, M; Dorigo, M; Dorigo, T; Dubey, A; Dudko, L.V; Duggan, D; Duperrin, A; Dutt, S; Dyshkant, A; Eads, M; Ebina, K; Edmunds, D; Elagin, A; Ellison, J; Elvira, V.D; Enari, Y; Eppig, A; Erbacher, R; Errede, S; Ershaidat, N; Eusebi, R; Evans, H; Evdokimov, A; Evdokimov, V.N; Facini, G; Farrington, S; Feindt, M; Feng, L; Ferbel, T; Fernandez, J.P; Fiedler, F; Field, R; Filthaut, F; Fisher, W; Fisk, H.E; Flanagan, G; Forrest, R; Fortner, M; Fox, H; Frank, M.J; Franklin, M; Freeman, J.C; Fuess, S; Funakoshi, Y; Furic, I; Gallinaro, M; Garcia-Bellido, A; Garcia, J.E; Garcia-Gonzalez, J.A; Garcia-Guerra, G.A; Garfinkel, A.F; Garosi, P; Gavrilov, V; Gay, P; Geng, W; Gerbaudo, D; Gerber, C.E; Gerberich, H; Gerchtein, E; Gershtein, Y; Giagu, S; Giakoumopoulou, V; Giannetti, P; Gibson, K; Ginsburg, C.M; Ginther, G; Giokaris, N; Giromini, P; Giurgiu, G; Glagolev, V; Glenzinski, D; Gold, M; Goldin, D; Goldschmidt, N; Golossanov, A; Golovanov, G; Gomez-Ceballos, G; Gomez, G; Goncharov, M; Gonzalez, O; Gorelov, I; Goshaw, A.T; Goulianos, K; Goussiou, A; Grannis, P.D; Greder, S; Greenlee, H; Grenier, G; Grinstein, S; Gris, Ph; Grivaz, J.F; Grohsjean, A; Grosso-Pilcher, C; Group, R.C; Grunendahl, S; Grunewald, M.W; Guillemin, T; Guimaraes da Costa, J; Gutierrez, G; Gutierrez, P; Hagopian, S; Hahn, S.R; Haley, J; Halkiadakis, E; Hamaguchi, A; Han, J.Y; Han, L; Happacher, F; Hara, K; Harder, K; Hare, D; Hare, M; Harel, A; Harr, R.F; Hatakeyama, K; Hauptman, J.M; Hays, C; Hays, J; Head, T; Hebbeker, T; Heck, M; Hedin, D; Hegab, H; Heinrich, J; Heinson, A.P; Heintz, U; Hensel, C; La Cruz, I.Heredia-De; Herndon, M; Herner, K; Hesketh, G; Hewamanage, S; Hildreth, M.D; Hirosky, R; Hoang, T; Hobbs, J.D; Hocker, A; Hoeneisen, B; Hogan, J; Hohlfeld, M; Hopkins, W; Horn, D; Hou, S; Howley, I; Hubacek, Z; Hughes, R.E; Hurwitz, M; Husemann, U; Hussain, N; Hussein, M; Huston, J; Hynek, V; Iashvili, I; Ilchenko, Y; Illingworth, R; Introzzi, G; Iori, M; Ito, A.S; Ivanov, A; Jabeen, S; Jaffre, M; James, E; Jang, D; Jayasinghe, A; Jayatilaka, B; Jeon, E.J; Jeong, M.S; Jesik, R; Jindariani, S; Johns, K; Johnson, E; Johnson, M; Jonckheere, A; Jones, M; Jonsson, P; Joo, K.K; Joshi, J; Jun, S.Y; Jung, A.W; Junk, T.R; Juste, A; Kaadze, K; Kajfasz, E; Kamon, T; Karchin, P.E; Karmanov, D; Kasmi, A; Kasper, P.A; Kato, Y; Katsanos, I; Kehoe, R; Kermiche, S; Ketchum, W; Keung, J; Khalatyan, N; Khanov, A; Kharchilava, A; Kharzheev, Y.N; Khotilovich, V; Kilminster, B; Kim, D.H; Kim, H.S; Kim, J.E; Kim, M.J; Kim, S.B; Kim, S.H; Kim, Y.J; Kim, Y.K; Kimura, N; Kirby, M; Kiselevich, I; Klimenko, S; Knoepfel, K; Kohli, J.M; Kondo, K; Kong, D.J; Konigsberg, J; Kotwal, A.V; Kozelov, A.V; Kraus, J; Kreps, M; Kroll, J; Krop, D; Kruse, M; Krutelyov, V; Kuhr, T; Kulikov, S; Kumar, A; Kupco, A; Kurata, M; Kurca, T; Kuzmin, V.A; Kwang, S; Laasanen, A.T; Lami, S; Lammel, S; Lammers, S; Lancaster, M; Lander, R.L; Landsberg, G; Lannon, K; Lath, A; Latino, G; Lebrun, P; LeCompte, T; Lee, E; Lee, H.S; Lee, H.S; Lee, J.S; Lee, S.W; Lee, S.W; Lee, W.M; Lei, X; Lellouch, J; Leo, S; Leone, S; Lewis, J.D; Li, H; Li, L; Li, Q.Z; Lim, J.K; Limosani, A; Lincoln, D; Lin, C.J; Lindgren, M; Linnemann, J; Lipaev, V.V; Lipeles, E; Lipton, R; Lister, A; Litvintsev, D.O; Liu, C; Liu, H; Liu, H; Liu, Q; Liu, T; Liu, Y; Lobodenko, A; Lockwitz, S; Loginov, A; Lokajicek, M; Lopes de Sa, R; Lubatti, H.J; Lucchesi, D; Lueck, J; Lujan, P; Lukens, P; Luna-Garcia, R; Lungu, G; Lyon, A.L; Lysak, R; Lys, J; Maciel, A.K.A; Madar, R; Madrak, R; Maeshima, K; Maestro, P; Magana-Villalba, R; Malik, S; 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    2012-01-01

    The combination of searches performed by the CDF and D0 collaborations at the Fermilab Tevatron Collider for neutral Higgs bosons produced in association with b quarks is reported. The data, corresponding to 2.6 fb-1 of integrated luminosity at CDF and 5.2 fb-1 at D0, have been collected in final states containing three or more b jets. Upper limits are set on the cross section multiplied by the branching ratio varying between 44 pb and 0.7 pb in the Higgs boson mass range 90 to 300 GeV, assuming production of a narrow scalar boson. Significant enhancements to the production of Higgs bosons can be found in theories beyond the standard model, for example in supersymmetry. The results are interpreted as upper limits in the parameter space of the minimal supersymmetric standard model in a benchmark scenario favoring this decay mode.

  1. Combination of measurements of the top-quark pair production cross section from the Tevatron Collider

    CERN Document Server

    Aaltonen, Timo Antero; Abbott, Braden Keim; Acharya, Bannanje Sripath; Adams, Mark Raymond; Adams, Todd; Agnew, James P; Alexeev, Guennadi D; Alkhazov, Georgiy D; Alton, Andrew K; Amerio, Silvia; Amidei, Dante E; Anastassov, Anton Iankov; Annovi, Alberto; Antos, Jaroslav; Apollinari, Giorgio; Appel, Jeffrey A; Arisawa, Tetsuo; Artikov, Akram Muzafarovich; Asaadi, Jonathan A; Ashmanskas, William Joseph; Askew, Andrew Warren; Atkins, Scott; Auerbach, Benjamin; Augsten, Kamil; Aurisano, Adam J; Avila, Carlos A; Azfar, Farrukh A; Badaud, Frederique; Badgett, William Farris; Bae, Taegil; Bagby, Linda F; Baldin, Boris; Bandurin, Dmitry V; Banerjee, Sunanda; Barbaro-Galtieri, Angela; Barberis, Emanuela; Baringer, Philip S; Barnes, Virgil E; Barnett, Bruce Arnold; Barria, Patrizia; Bartlett, JFrederick; Bartos, Pavol; Bassler, Ursula Rita; Bauce, Matteo; Bazterra, Victor; Bean, Alice L; Bedeschi, Franco; Begalli, Marcia; Behari, Satyajit; Bellantoni, Leo; Bellettini, Giorgio; Bellinger, James Nugent; Benjamin, Douglas P; Beretvas, Andrew F; Beri, Suman B; Bernardi, Gregorio; Bernhard, Ralf Patrick; Bertram, Iain A; Besancon, Marc; Beuselinck, Raymond; Bhat, Pushpalatha C; Bhatia, Sudeep; Bhatnagar, Vipin; Bhatti, Anwar Ahmad; Bland, Karen Renee; Blazey, Gerald Charles; Blessing, Susan K; Bloom, Kenneth A; Blumenfeld, Barry J; Bocci, Andrea; Bodek, Arie; Boehnlein, Amber S; Boline, Daniel Dooley; Boos, Edward E; Borissov, Guennadi; Bortoletto, Daniela; Boudreau, Joseph Francis; Boveia, Antonio; Brandt, Andrew; Brandt, Oleg; Brigliadori, Luca; Brock, Raymond L; Bromberg, Carl Michael; Bross, Alan D; Brown, Duncan Paul; Brucken, Erik; Bu, Xue-Bing; Budagov, Ioulian A; Budd, Howard Scott; Buehler, Marc; Buescher, Volker; Bunichev, Viacheslav Yevgenyevich; Burdin, Sergey; Burkett, Kevin Alan; Busetto, Giovanni; Bussey, Peter John; Buszello, Claus Peter; Butti, Pierfrancesco; Buzatu, Adrian; Calamba, Aristotle; Camacho-Perez, Enrique; Camarda, Stefano; Campanelli, Mario; Canelli, Florencia; Carls, Benjamin; Carlsmith, Duncan L; Carosi, Roberto; Carrillo Moreno, Salvador; Casal Larana, Bruno; Casarsa, Massimo; Casey, Brendan Cameron Kieran; Castilla-Valdez, Heriberto; Castro, Andrea; Catastini, Pierluigi; Caughron, Seth Aaron; Cauz, Diego; Cavaliere, Viviana; Cavalli-Sforza, Matteo; Cerri, Alessandro; Cerrito, Lucio; Chakrabarti, Subhendu; Chan, Kwok Ming Leo; Chandra, Avdhesh; Chapon, Emilien; Chen, Guo; Chen, Yen-Chu; Chertok, Maxwell Benjamin; Chiarelli, Giorgio; Chlachidze, Gouram; Cho, Kihyeon; Cho, Sung-Woong; Choi, Suyong; Chokheli, Davit; Choudhary, Brajesh C; Cihangir, Selcuk; Claes, Daniel R; Clark, Allan Geoffrey; Clarke, Christopher Joseph; Clutter, Justace Randall; Convery, Mary Elizabeth; Conway, John Stephen; Cooke, Michael P; Cooper, William Edward; Corbo, Matteo; Corcoran, Marjorie D; Cordelli, Marco; Couderc, Fabrice; Cousinou, Marie-Claude; Cox, Charles Alexander; Cox, David Jeremy; Cremonesi, Matteo; Cruz Alonso, Daniel; Cuevas Maestro, Javier; Culbertson, Raymond Lloyd; Cutts, David; Das, Amitabha; D'Ascenzo, Nicola; Datta, Mousumi; Davies, Gavin John; de Barbaro, Pawel; de Jong, Sijbrand Jan; De La Cruz-Burelo, Eduard; Deliot, Frederic; Demina, Regina; Demortier, Luc M; Deninno, Maria Maddalena; Denisov, Dmitri S; Denisov, Sergei P; D'Errico, Maria; Desai, Satish Vijay; Deterre, Cecile; DeVaughan, Kayle Otis; Devoto, Francesco; Di Canto, Angelo; Di Ruzza, Benedetto; Diehl, HThomas; Diesburg, Michael; Ding, Pengfei; Dittmann, Jay Richard; Dominguez, D. 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Hays, Christopher Paul; Hays, Jonathan M; Head, Tim; Hebbeker, Thomas; Hedin, David R; Hegab, Hatim; Heinrich, Joel G; Heinson, Ann; Heintz, Ulrich; Hensel, Carsten; Heredia-De La Cruz, Ivan; Herndon, Matthew Fairbanks; Herner, Kenneth Richard; Hesketh, Gavin G; Hildreth, Michael D; Hirosky, Robert James; Hoang, Trang; Hobbs, John D; Hocker, James Andrew; Hoeneisen, Bruce; Hogan, Julie; Hohlfeld, Mark; Holzbauer, Jenny Lyn; Hong, Ziqing; Hopkins, Walter Howard; Hou, Suen Ray; Howley, Ian James; Hubacek, Zdenek; Hughes, Richard Edward; Husemann, Ulrich; Hussein, Mohammad; Huston, Joey Walter; Hynek, Vlastislav; Iashvili, Ia; Ilchenko, Yuriy; Illingworth, Robert A; Introzzi, Gianluca; Iori, Maurizio; Ito, Albert S; Ivanov, Andrew Gennadievich; Jabeen, Shabnam; Jaffre, Michel J; James, Eric B; Jang, Dongwook; Jayasinghe, Ayesh; Jayatilaka, Bodhitha Anjalike; Jeon, Eun-Ju; Jeong, Min-Soo; Jesik, Richard L; Jiang, Peng; Jindariani, Sergo Robert; Johns, Kenneth Arthur; Johnson, Emily; Johnson, Marvin E; Jonckheere, Alan M; Jones, Matthew T; Jonsson, Per Martin; Joo, Kyung Kwang; Joshi, Jyoti; Jun, Soon Yung; Jung, Andreas Werner; Junk, Thomas R; Juste, Aurelio; Kajfasz, Eric; Kambeitz, Manuel; Kamon, Teruki; Karchin, Paul Edmund; Karmanov, Dmitriy Y; Kasmi, Azeddine; Kato, Yukihiro; Katsanos, Ioannis; Kehoe, Robert Leo Patrick; Kermiche, Smain; Ketchum, Wesley Robert; Keung, Justin Kien; Khalatyan, Norayr; Khanov, Alexander; Kharchilava, Avto; Kharzheev, Yuri N; Kilminster, Benjamin John; Kim, DongHee; Kim, Hyunsoo; Kim, Jieun; Kim, Min Jeong; Kim, Shin-Hong; Kim, Soo Bong; Kim, Young-Jin; Kim, Young-Kee; Kimura, Naoki; Kirby, Michael H; Kiselevich, Ivan Lvovich; Knoepfel, Kyle James; Kohli, Jatinder M; Kondo, Kunitaka; Kong, Dae Jung; Konigsberg, Jacobo; Kotwal, Ashutosh Vijay; Kozelov, Alexander V; Kraus, James Alexander; Kreps, Michal; Kroll, IJoseph; Kruse, Mark Charles; Kuhr, Thomas; Kumar, Ashish; Kupco, Alexander; Kurata, Masakazu; Kurca, Tibor; Kuzmin, Valentin Alexandrovich; Laasanen, Alvin Toivo; Lammel, Stephan; Lammers, Sabine Wedam; Lancaster, Mark; Lannon, Kevin Patrick; Latino, Giuseppe; Lebrun, Patrice; Lee, Hyeon-Seung; Lee, Hyun Su; Lee, Jaison; Lee, Seh-Wook; Lee, William M; Lei, Xiaowen; Lellouch, Jeremie; Leo, Sabato; Leone, Sandra; Lewis, Jonathan D; Li, Dikai; Li, Hengne; Li, Liang; Li, Qi-Zhong; Lim, Jeong Ku; Limosani, Antonio; Lincoln, Donald W; Linnemann, James Thomas; Lipaev, Vladimir V; Lipeles, Elliot David; Lipton, Ronald J; Lister, Alison; Liu, Hao; Liu, Huanzhao; Liu, Qiuguang; Liu, Tiehui Ted; Liu, Yanwen; Lobodenko, Alexandre; Lockwitz, Sarah E; Loginov, Andrey Borisovich; Lokajicek, Milos; Lopes de Sa, Rafael; Lucchesi, Donatella; Lucà, Alessandra; Lueck, Jan; Lujan, Paul Joseph; Lukens, Patrick Thomas; Luna-Garcia, Rene; Lungu, Gheorghe; Lyon, Adam Leonard; Lys, Jeremy E; Lysak, Roman; Maciel, Arthur KA; Madar, Romain; Madrak, Robyn Leigh; Maestro, Paolo; Magana-Villalba, Ricardo; Malik, Sarah Alam; Malik, Sudhir; Malyshev, Vladimir L; Manca, Giulia; Manousakis-Katsikakis, Arkadios; Mansour, Jason; Marchese, Luigi Marchese; Margaroli, Fabrizio; Marino, Christopher Phillip; Martinez-Ortega, Jorge; Martínez-Perez, Mario; Matera, Keith; Mattson, Mark Edward; Mazzacane, Anna; Mazzanti, Paolo; McCarthy, Robert L; Mcgivern, Carrie Lynne; McNulty, Ronan; Mehta, Andrew; Mehtala, Petteri; Meijer, Melvin M; Melnitchouk, Alexander S; Menezes, Diego D; Mercadante, Pedro Galli; Merkin, Mikhail M; Mesropian, Christina; Meyer, Arnd; Meyer, Jorg Manfred; Miao, Ting; Miconi, Florian; Mietlicki, David John; Mitra, Ankush; Miyake, Hideki; Moed, Shulamit; Moggi, Niccolo; Mondal, Naba K; Moon, Chang-Seong; Moore, Ronald Scott; Morello, Michael Joseph; Mukherjee, Aseet; Mulhearn, Michael James; Muller, Thomas; Murat, Pavel A; Mussini, Manuel; Nachtman, Jane Marie; Nagai, Yoshikazu; Naganoma, Junji; Nagy, Elemer; Nakano, Itsuo; Napier, Austin; Narain, Meenakshi; Nayyar, Ruchika; Neal, Homer A; Negret, Juan Pablo; Nett, Jason Michael; Neu, Christopher Carl; Neustroev, Petr V; Nguyen, Huong Thi; Nigmanov, Turgun S; Nodulman, Lawrence J; Noh, Seoyoung; Norniella Francisco, Olga; Nunnemann, Thomas P; Oakes, Louise Beth; Oh, Seog Hwan; Oh, Young-do; Oksuzian, Iuri Artur; Okusawa, Toru; Orava, Risto Olavi; Hernandez Orduna, Jose de Jesus; Ortolan, Lorenzo; Osman, Nicolas Ahmed; Osta, Jyotsna; Pagliarone, Carmine Elvezio; Pal, Arnab; Palencia, Jose Enrique; Palni, Prabhakar; Papadimitriou, Vaia; Parashar, Neeti; Parihar, Vivek; Park, Sung Keun; Parker, William Chesluk; Partridge, Richard A; Parua, Nirmalya; Patwa, Abid; Pauletta, Giovanni; Paulini, Manfred; Paus, Christoph Maria Ernst; Penning, Bjoern; Perfilov, Maxim Anatolyevich; Peters, Reinhild Yvonne Fatima; Petridis, Konstantinos; Petrillo, Gianluca; Petroff, Pierre; Phillips, Thomas J; Piacentino, Giovanni M; Pianori, Elisabetta; Pilot, Justin Robert; Pitts, Kevin T; Plager, Charles; Pleier, Marc-Andre; Podstavkov, Vladimir M; Pondrom, Lee G; Popov, Alexey V; Poprocki, Stephen; Potamianos, Karolos Jozef; Pranko, Aliaksandr Pavlovich; Prewitt, Michelle; Price, Darren; Prokopenko, Nikolay N; Prokoshin, Fedor; Ptohos, Fotios K; Punzi, Giovanni; Qian, Jianming; Quadt, Arnulf; Quinn, Breese; Ranjan, Niharika; Ratoff, Peter N; Razumov, Ivan A; Redondo Fernández, Ignacio; Renton, Peter B; Rescigno, Marco; Rimondi, Franco; Ripp-Baudot, Isabelle; Ristori, Luciano; Rizatdinova, Flera; Robson, Aidan; Rodriguez, Tatiana Isabel; Rolli, Simona; Rominsky, Mandy Kathleen; Ronzani, Manfredi; Roser, Robert Martin; Rosner, Jonathan L; Ross, Anthony; Royon, Christophe; Rubinov, Paul Michael; Ruchti, Randal C; Ruffini, Fabrizio; Ruiz Jimeno, Alberto; Russ, James S; Rusu, Vadim Liviu; Sajot, Gerard; Sakumoto, Willis Kazuo; Sakurai, Yuki; Sanchez-Hernandez, Alberto; Sanders, Michiel P; Santi, Lorenzo; Santos, Angelo Souza; Sato, Koji; Savage, David G; Saveliev, Valeri; Savoy-Navarro, Aurore; Sawyer, HLee; Scanlon, Timothy P; Schamberger, RDean; Scheglov, Yury A; Schellman, Heidi M; Schlabach, Philip; Schmidt, Eugene E; Schwanenberger, Christian; Schwarz, Thomas A; Schwienhorst, Reinhard H; Scodellaro, Luca; Scuri, Fabrizio; Seidel, Sally C; Seiya, Yoshihiro; Sekaric, Jadranka; Semenov, Alexei; Severini, Horst; Sforza, Federico; Shabalina, Elizaveta K; Shalhout, Shalhout Zaki; Shary, Viacheslav V; Shaw, Savanna; Shchukin, Andrey A; Shears, Tara G; Shepard, Paul F; Shimojima, Makoto; Shochet, Melvyn J; Shreyber-Tecker, Irina; Simak, Vladislav J; Simonenko, Alexander V; Skubic, Patrick Louis; Slattery, Paul F; Sliwa, Krzysztof Jan; Smirnov, Dmitri V; Smith, John Rodgers; Snider, Frederick Douglas; Snow, Gregory R; Snow, Joel Mark; Snyder, Scott Stuart; Soldner-Rembold, Stefan; Song, Hao; Sonnenschein, Lars; Sorin, Maria Veronica; Soustruznik, Karel; St Denis, Richard Dante; Stancari, Michelle Dawn; Stark, Jan; Stentz, Dale James; Stoyanova, Dina A; Strauss, Michael G; Strologas, John; Sudo, Yuji; Sukhanov, Alexander I; Suslov, Igor M; Suter, Louise; Svoisky, Peter V; Takemasa, Ken-ichi; Takeuchi, Yuji; Tang, Jian; Tecchio, Monica; Teng, Ping-Kun; Thom, Julia; Thomson, Evelyn Jean; Thukral, Vaikunth; Titov, Maxim; Toback, David A; Tokar, Stanislav; Tokmenin, Valeriy V; Tollefson, Kirsten Anne; Tomura, Tomonobu; Tonelli, Diego; Torre, Stefano; Torretta, Donatella; Totaro, Pierluigi; Trovato, Marco; Tsai, Yun-Tse; Tsybychev, Dmitri; Tuchming, Boris; Tully, Christopher George T; Ukegawa, Fumihiko; Uozumi, Satoru; Uvarov, Lev; Uvarov, Sergey L; Uzunyan, Sergey A; Van Kooten, Richard J; van Leeuwen, Willem M; Varelas, Nikos; Varnes, Erich W; Vasilyev, Igor A; Vázquez-Valencia, Elsa Fabiola; Velev, Gueorgui; Vellidis, Konstantinos; Verkheev, Alexander Yurievich; Vernieri, Caterina; Vertogradov, Leonid S; Verzocchi, Marco; Vesterinen, Mika; Vidal Marono, Miguel; Vilanova, Didier; Vilar Cortabitarte, Rocio; Vizán Garcia, Jesus Manuel; Vogel, Marcelo; Vokac, Petr; Volpi, Guido; Wagner, Peter; Wahl, Horst D; Wallny, Rainer S; Wang, Michael HLS; Wang, Song-Ming; Warchol, Jadwiga; Waters, David S; Watts, Gordon Thomas; Wayne, Mitchell R; Weichert, Jonas; Welty-Rieger, Leah Christine; Wester, William Carl; Whiteson, Daniel O; Wicklund, Arthur Barry; Wilbur, Scott; Williams, Hugh H; Williams, Mark Richard James; Wilson, Graham Wallace; Wilson, Jonathan Samuel; Wilson, Peter James; Winer, Brian L; Wittich, Peter; Wobisch, Markus; Wolbers, Stephen A; Wolfe, Homer; Wood, Darien Robert; Wright, Thomas Roland; Wu, Xin; Wu, Zhenbin; Wyatt, Terence R; Xie, Yunhe; Yamada, Ryuji; Yamamoto, Kazuhiro; Yamato, Daisuke; Yang, Siqi; Yang, Tingjun; Yang, Un-Ki; Yang, Yu Chul; Yao, Wei-Ming; Yasuda, Takahiro; Yatsunenko, Yuriy A; Ye, Wanyu; Ye, Zhenyu; Yeh, Gong Ping; Yi, Kai; Yin, Hang; Yip, Kin; Yoh, John; Yorita, Kohei; Yoshida, Takuo; Youn, Sungwoo; Yu, Geum Bong; Yu, Intae; Yu, Jiaming; Zanetti, Anna Maria; Zeng, Yu; Zennamo, Joseph; Zhao, Tianqi Gilbert; Zhou, Bing; Zhou, Chen; Zhu, Junjie; Zielinski, Marek; Zieminska, Daria; Zivkovic, Lidija; Zucchelli, Stefano

    2014-01-01

    We combine six measurements of the inclusive top-quark pair (ttbar) production cross section (sigma_ttbar) from data collected with the CDF and D0 detectors at the Fermilab Tevatron with proton anti-proton collisions at sqrt{s} = 1.96 TeV. The data correspond to integrated luminosities of up to 8.8 fb^{-1}. We obtain a value of sigma_ttbar = 7.60 \\pm 0.41 pb for a top-quark mass of m_t=172.5 GeV. The contributions to the uncertainty are 0.20 pb from statistical sources, 0.29 pb from systematic sources, and 0.21 pb from the uncertainty on the integrated luminosity. The result is in good agreement with the standard model expectation of 7.35^{+0.28}_{-0.33} pb at NNLO+NNLL in pertubative QCD.

  2. Polarization for prompt J/ψ and ψ(2s) production at the Tevatron and LHC.

    Science.gov (United States)

    Gong, Bin; Wan, Lu-Ping; Wang, Jian-Xiong; Zhang, Hong-Fei

    2013-01-25

    With nonrelativistic QCD factorization, we present the first complete next-to-leading order study on the polarization of prompt J/ψ hadroproduction by including feeddown from χ(c)((3)P(J)(1),(3)S(1)(8)) and ψ(2s) which turn out to be very important parts. By using the color-octet long-distance matrix elements obtained from a combined fit of the measurements at the Tevatron and LHC for J/ψ, ψ(2s) and χ(c), the prompt J/ψ polarization predictions are presented, and the results are in agreement with the CDF run I data (except two points), but in conflict with the CDF run II data, while they are close to the ALICE data (inclusive J/ψ). The measurements at the LHC are expected to clarify the situation.

  3. Status of the observed and predicted b anti-b production at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Happacher, F.; Giromini, P.; /Frascati; Ptohos, F.; /Cyprus U.

    2005-09-01

    The authors review the experimental status of the b-quark production at the Fermilab Tevatron. They compare all available measurements to perturbative QCD predictions (NLO and FONLL) and also to the parton-level cross section evaluated with parton-shower Monte Carlo generators. They examine both the single b cross section and the so called b{bar b} correlations. The review shows that the experimental situation is quite complicated because the measurements appear to be inconsistent among themselves. In this situation, there is no solid basis to either claim that perturbative QCD is challenged by these measurements or, in contrast, that long-standing discrepancies between data and theory have been resolved by incrementally improving the measurements and the theoretical prediction.

  4. Benchmarks for the Forward Observables at RHIC, the Tevatron-run II and the LHC

    CERN Document Server

    Cudell, J R; Gauron, P; Kang, K; Kuyanov, Yu V; Lugovsky, S B; Martynov, E S; Nicolescu, Basarab; Razuvaev, E A; Tkachenko, N P; Kuyanov, Yu.V.

    2002-01-01

    We present predictions on the total cross sections and on the ratio of the real part to the imaginary part of the elastic amplitude (rho parameter) for present and future pp and pbar p colliders, and on total cross sections for gamma p -> hadrons at cosmic-ray energies and for gamma gamma-> hadrons up to sqrt{s}=1 TeV. These predictions are based on an extensive study of possible analytic parametrisations invoking the biggest hadronic dataset available at t=0. The uncertainties on total cross sections, including the systematic errors due to contradictory data points from FNAL, can reach 1.9% at RHIC, 3.1% at the Tevatron, and 4.8% at the LHC, whereas those on the rho parameter are respectively 5.4%, 5.2%, and 5.4%.

  5. Forward observables at RHIC, the Tevatron run II and the LHC

    CERN Document Server

    Cudell, J R; Gauron, P; Kang, K; Kuyanov, Yu V; Lugovsky, S B; Martynov, E S; Nicolescu, Basarab; Razuvaev, E A; Tkachenko, N P; Kuyanov, Yu.V.

    2002-01-01

    We present predictions on the total cross sections and on the ratio of the real part to the imaginary part of the elastic amplitude (rho parameter) for present and future pp and pbar p colliders, and on total cross sections for gamma p -> hadrons at cosmic-ray energies and for gamma gamma -> hadrons up to sqrt(s)=1 TeV. These predictions are based on a study of many possible analytic parametrisations and invoke the current hadronic dataset at t=0. The uncertainties on total cross sections, including the systematic theoretical errors, reach 1% at RHIC, 3% at the Tevatron, and 10% at the LHC, whereas those on the rho parameter are respectively 10%, 17%, and 26%.

  6. First Observation of Vector Boson Pairs in a Hadronic Final State at the Tevatron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Aaltonen, T.; /Helsinki Inst. of Phys.; Adelman, Jahred A.; /Chicago U., EFI; Akimoto, T.; /Tsukuba U.; Alvarez Gonzalez, B.; /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, Dante E.; /Michigan U.; Anastassov, A.; /Northwestern U.; Annovi, Alberto; /Frascati; Antos, Jaroslav; /Comenius U.; Apollinari, G.; /Fermilab; Apresyan, A.; /Purdue U. /Waseda U.

    2009-05-01

    We present the first observation in hadronic collisions of the electroweak production of vector boson pairs (VV, V = W,Z) where one boson decays to a dijet final state. The data correspond to 3.5 fb{sup -1} of integrated luminosity of p{bar p} collisions at {radical}s = 1.96 TeV collected by the CDF II detector at the Fermilab Tevatron. We observe 1516 {+-} 239(stat) {+-} 144(syst) diboson candidate events and measure a cross section {sigma}(p{bar p} {yields} VV + X) of 18.0 {+-} 2.8(stat) {+-} 2.4(syst) {+-} 1.1(lumi) pb, in agreement with the expectations of the standard model.

  7. NNLO QCD predictions for fully-differential top-quark pair production at the Tevatron

    CERN Document Server

    Czakon, Michal; Heymes, David; Mitov, Alexander

    2016-01-01

    We present a comprehensive study of differential distributions for Tevatron top-pair events at the level of stable top quarks. All calculations are performed in NNLO QCD with the help of a fully differential partonic Monte-Carlo and are exact at this order in perturbation theory. We present predictions for all kinematic distributions for which data exists. Particular attention is paid on the top-quark forward-backward asymmetry which we study in detail. We compare the NNLO results with existing approximate NNLO predictions as well as differential distributions computed with different parton distribution sets. Theory errors are significantly smaller than current experimental ones with overall agreement between theory and data.

  8. Exploring the Yukawa unified minimal supergravity model at the Tevatron, LEP II, and the LHC

    CERN Document Server

    Gunion, J F

    1994-01-01

    We explore the prospects for detection of sparticles and Higgs bosons at the Tevatron, LEP-200 and the LHC in the allowed parameter space of a "Yukawa unified" ($\\lambda_b(M_U)=\\lambda_{\\ tau}(M_U)$) minimal supergravity (YUMS) model, where the only non-zero unification scale soft-SUSY-breaking terms are a universal gaugino mass and a Higgs mixing term. In a bottom-up approach, just two weak scale parameters, $\\tanb$ and $\\mha$ (along with the sign of the Higgs mixing parameter $\\mu$) completely parameterize the model. Many interesting "special" situations regarding sparticle and Higgs discovery arise, such as the importance of the invisible $\\hl\\rta\\cnone\\cnone,\\snu\\ snubar$ decay modes.

  9. First observation of vector boson pairs in a hadronic final state at the tevatron collider.

    Science.gov (United States)

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Margaroli, F; Marino, C; Marino, C P; Martin, A; Martin, V; Martínez, M; Martínez-Ballarín, R; Maruyama, T; Mastrandrea, P; Masubuchi, T; Mathis, M; Mattson, M E; Mazzanti, P; McFarland, K S; McIntyre, P; McNulty, R; Mehta, A; Mehtala, P; Menzione, A; Merkel, P; Mesropian, C; Miao, T; Miladinovic, N; Miller, R; Mills, C; Milnik, M; Mitra, A; Mitselmakher, G; Miyake, H; Moggi, N; Mondragon, M N; Moon, C S; Moore, R; Morello, M J; Morlock, J; Fernandez, P Movilla; Mülmenstädt, J; Mukherjee, A; Muller, Th; Mumford, R; Murat, P; Mussini, M; Nachtman, J; Nagai, Y; Nagano, A; Naganoma, J; Nakamura, K; Nakano, I; Napier, A; Necula, V; Nett, J; Neu, C; Neubauer, M S; Neubauer, S; Nielsen, J; Nodulman, L; Norman, M; Norniella, O; Nurse, E; Oakes, L; Oh, S H; Oh, Y D; Oksuzian, I; Okusawa, T; Orava, R; Osterberg, K; Griso, S Pagan; Palencia, E; Papadimitriou, V; Papaikonomou, A; Paramonov, A A; Parks, B; Pashapour, S; Patrick, J; Pauletta, G; Paulini, M; Paus, C; Peiffer, T; Pellett, D E; Penzo, A; Phillips, T J; Piacentino, G; Pianori, E; Pinera, L; Pitts, K; Plager, C; Pondrom, L; Poukhov, O; Pounder, N; Prakoshyn, F; Pronko, A; Proudfoot, J; Ptohos, F; Pueschel, E; Punzi, G; Pursley, J; Rademacker, J; Rahaman, A; Ramakrishnan, V; Ranjan, N; Redondo, I; Renton, P; Renz, M; Rescigno, M; Richter, S; Rimondi, F; Ristori, L; Robson, A; Rodrigo, T; Rodriguez, T; Rogers, E; Rolli, S; Roser, R; Rossi, M; Rossin, R; Roy, P; Ruiz, A; Russ, J; Rusu, V; Rutherford, B; Saarikko, H; Safonov, A; Sakumoto, W K; Saltó, O; Santi, L; Sarkar, S; Sartori, L; Sato, K; Savoy-Navarro, A; Schlabach, P; Schmidt, A; Schmidt, E E; Schmidt, M A; Schmidt, M P; Schmitt, M; Schwarz, T; Scodellaro, L; Scribano, A; Scuri, F; Sedov, A; Seidel, S; Seiya, Y; Semenov, A; Sexton-Kennedy, L; Sforza, F; Sfyrla, A; Shalhout, S Z; Shears, T; Shepard, P F; Shimojima, M; Shiraishi, S; Shochet, M; Shon, Y; Shreyber, I; Sinervo, P; Sisakyan, A; Slaughter, A J; Slaunwhite, J; Sliwa, K; Smith, J R; Snider, F D; Snihur, R; Soha, A; Somalwar, S; Sorin, V; Spreitzer, T; Squillacioti, P; Stanitzki, M; St Denis, R; Stelzer, B; Stelzer-Chilton, O; Stentz, D; Strologas, J; Strycker, G L; Suh, J S; Sukhanov, A; Suslov, I; Suzuki, T; Taffard, A; Takashima, R; Takeuchi, Y; Tanaka, R; Tecchio, M; Teng, P K; Terashi, K; Thom, J; Thompson, A S; Thompson, G A; Thomson, E; Tipton, P; Ttito-Guzmán, P; Tkaczyk, S; Toback, D; Tokar, S; Tollefson, K; Tomura, T; Tonelli, D; Torre, S; Torretta, D; Totaro, P; Tourneur, S; Trovato, M; Tsai, S-Y; Tu, Y; Turini, N; Ukegawa, F; Vallecorsa, S; van Remortel, N; Varganov, A; Vataga, E; Vázquez, F; Velev, G; Vellidis, C; Vidal, M; Vidal, R; Vila, I; Vilar, R; Vine, T; Vogel, M; Volobouev, I; Volpi, G; Wagner, P; Wagner, R G; Wagner, R L; Wagner, W; Wagner-Kuhr, J; Wakisaka, T; Wallny, R; Wang, S M; Warburton, A; Waters, D; Weinberger, M; Weinelt, J; Wester, W C; Whitehouse, B; Whiteson, D; Wicklund, A B; Wicklund, E; Wilbur, S; Williams, G; Williams, H H; Wilson, P; Winer, B L; Wittich, P; Wolbers, S; Wolfe, C; Wright, T; Wu, X; Würthwein, F; Xie, S; Yagil, A; Yamamoto, K; Yamaoka, J; Yang, U K; Yang, Y C; Yao, W M; Yeh, G P; Yi, K; Yoh, J; Yorita, K; Yoshida, T; Yu, G B; Yu, I; Yu, S S; Yun, J C; Zanello, L; Zanetti, A; Zhang, X; Zheng, Y; Zucchelli, S

    2009-08-28

    We present the first observation in hadronic collisions of the electroweak production of vector boson pairs (VV, V = W, Z) where one boson decays to a dijet final state. The data correspond to 3.5 fb(-1) of integrated luminosity of pp[over ] collisions at sqrt[s] = 1.96 TeV collected by the CDF II detector at the Fermilab Tevatron. We observe 1516 + or - 239(stat) + or - 144(syst) diboson candidate events and measure a cross section sigma(pp[over ]-->VV + X) of 18.0 + or - 2.8(stat) + or - 2.4(syst) + or -1.1(lumi) pb, in agreement with the expectations of the standard model.

  10. Model-independent analysis of the Fermilab Tevatron turn-by-turn beam position monitor measurements

    Energy Technology Data Exchange (ETDEWEB)

    Petrenko, A.V.; /Novosibirsk, IYF; Valishev, A.A.; Lebedev, V.A.; /Fermilab

    2011-09-01

    Coherent transverse beam oscillations in the Tevatron were analyzed with the model-independent analysis (MIA) technique. This allowed one to obtain the model-independent values of coupled betatron amplitudes, phase advances, and dispersion function around the ring from a single dipole kick measurement. In order to solve the MIA mode mixing problem which limits the accuracy of determination of the optical functions, we have developed a new technique of rotational MIA mode untangling. The basic idea is to treat each beam position monitor (BPM) as two BPMs separated in a ring by exactly one turn. This leads to a simple criterion of MIA mode separation: the betatron phase advance between any BPM and its counterpart shifted by one turn should be equal to the betatron tune and therefore should not depend on the BPM position in the ring. Furthermore, we describe a MIA-based technique to locate vibrating magnets in a storage ring.

  11. W/Z + jets production at the tevatron {bar p}p collider

    Energy Technology Data Exchange (ETDEWEB)

    Yu, Jaehoon [University of Rochester, Rochester, NY (United States). Dept. of Physics and Astronomy

    1995-06-01

    Both the D0 and CDF experiments at Fermilab Tevatron collider at {radical}s = 1.8TeV have accumulated over 13pb{sup {minus}1} of data during the 1992--1993 collider run. Each experiment collected more than 10,000 W {yields} l + {nu} and 1,000 Z {yields} l + {bar l} candidates for each lepton species (e and {mu}). Using this large data sample of W and Z candidates, the two experiments are actively testing perturbative QCD predictions. Among the studies that are in progress, preliminary results of Z+jets characteristics, multiplicity distributions of associated jets, and a determination of the strong coupling constant using the ratio of the +ljet to W + Ojet cross sections are presented.

  12. Next-to-Leading Order QCD Predictions for Z, gamma^* 3-Jet Distributions at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Berger, C.F.; /MIT, LNS; Bern, Z.; /UCLA; Dixon, L.J.; /SLAC; Cordero, F.Febres; /Simon Bolivar U.; Forde, D.; /CERN /NIKHEF, Amsterdam; Gleisberg, T.; /SLAC; Ita, H.; /UCLA; Kosower, D.A.; /DAPNIA, Saclay; Maitre, D.; /Durham U.

    2010-06-02

    Using BlackHat in conjunction with SHERPA, we have computed next-to-leading order QCD predictions for a variety of distributions in Z, {gamma}{sup {asterisk}}+ 1, 2, 3-jet production at the Tevatron, where the Z boson or off-shell photon decays into an electron-positron pair. We find good agreement between the NLO results for jet {sub pT} distributions and measurements by CDF and D0. We also present jetproduction ratios, or probabilities of finding one additional jet. As a function of vector-boson {sub pT} , the ratios have distinctive features which we describe in terms of a simple model capturing leading logarithms and phase-space and parton-distribution-function suppression.

  13. Diffractive production of bb-bar in proton-antiproton collision at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Alves, G. [Centro Brasileiro de Pesquisas Fisicas (CBPF), Rio de Janeiro, RJ (Brazil); Levin, E. [Petersburg Nuclear Physics Inst. (Russian Federation). Thoery Dept.; Santoro, A. [Fermi National Accelerator Lab., Batavia, IL (United States)

    1996-08-01

    We show that the cross section of the diffractive production of b b-bar can be described as the sum of two contributions: the first is proportional to the probability of finding a small size b b-bar color dipole in the fast hadron wave function before the interaction with a target, while the second is the b b-bar production after or during the interaction with the target. The formulae are presented as well as the discussion of the interrelation between these two contributions and the Ingelman-Schlein and coherent diffraction mechanisms. The main prediction is that the coherent diffraction mechanism dominates, at least at the Tevatron energies, giving the unique possibility to study it experimentally. (author). 25 refs., 10 figs.

  14. Benchmarks for the forward observables at RHIC, the Tevatron-run II, and the LHC.

    Science.gov (United States)

    Cudell, J R; Ezhela, V V; Gauron, P; Kang, K; Kuyanov, Yu V; Lugovsky, S B; Martynov, E; Nicolescu, B; Razuvaev, E A; Tkachenko, N P

    2002-11-11

    We present predictions on the total cross sections and on the rho parameter for present and future pp and (-)pp colliders, and on total cross sections for gammap-->hadrons at cosmic-ray energies and for gammagamma-->hadrons up to sqrt[s]=1 TeV. These predictions are based on an extensive study of possible analytic parametrizations invoking the largest hadronic dataset available at t=0. The uncertainties on total cross sections reach 1.9% at the Relativistic Heavy Ion Collider, 3.1% at the Tevatron, and 4.8% at the Large Hadron Collider, whereas those on the rho parameter are, respectively, 5.4%, 5.2%, and 5.4%.

  15. Tales of the young top quark - Selected recent results from the LHC and Tevatron

    CERN Document Server

    Lister, Alison; The ATLAS collaboration

    2015-01-01

    After a short historical introduction of the discovery of the top quark 20 years ago, a brief motivation was given for continuing to study the heaviest known fundamental particle. Selected recent results from the ATLAS and CMS experiments at the LHC, and the CDF and D0 experiments at the Tevatron are presented. First measurements of the top mass, a fundamental parameter of the Standard Model, are presented. This is followed by stringent tests of the Standard model through the measurement of the \\ttbar\\ inclusive and differential cross-sections as well as the associated production of vector bosons. The spin correlation is used as an example to illustrate the relevance of prevision top quark properly measurements in the search for physics beyond the standard model. Finally some recent results in single top production are presented.

  16. Métastases gastro-intestinales du cancer du sein: à propos de 2 cas

    Science.gov (United States)

    Loubna, Mezouar; Mohamed, El Hfid; Tijani, El Harroudi; Fouzia, Ghadouani; Hanane, Haj Kacem; Zouhour, Bourhaleb; Asmae, Ouabdelmoumen

    2013-01-01

    Le cancer du sein est le cancer le plus fréquent chez la femme, notamment au Maroc, avec un taux de mortalité élevé. Les métastases gastro-intestinales d'un carcinome canalaire du sein sont rares. Leur diagnostic est difficile du fait de la nature non spécifique des symptômes. Nous rapportons deux observations originales de métastases gastroduodénales d'un cancer canalaire infiltrant du sein. Les métastases gastro-intestinales du cancer du sein sont très rares; la présence de symptômes gastro-intestinaux chez une malade ayant un antécédent de cancer du sein doit faire suspecter une atteinte métastatique gastro-intestinale. PMID:24198876

  17. Session du Conseil du CERN : le ministre britannique, Robert Jackson, souligne l'intérêt de on pays pour l'avenir du CERN : décisions du Conseil pour la mise en oeuvre des recommandations du Comité d'évaluation du CERN: départ anticipé pour 200 membres au moins du personnel - mise à jour de la méthode de calcule pour les contributions des Etats Membres au budget

    CERN Multimedia

    CERN Press Office. Geneva

    1988-01-01

    Session du Conseil du CERN : le ministre britannique, Robert Jackson, souligne l'intérêt de on pays pour l'avenir du CERN : décisions du Conseil pour la mise en oeuvre des recommandations du Comité d'évaluation du CERN: départ anticipé pour 200 membres au moins du personnel - mise à jour de la méthode de calcule pour les contributions des Etats Membres au budget

  18. Des Taiwanais dans Ie sud du Fujian

    Institute of Scientific and Technical Information of China (English)

    2002-01-01

    Se trouvant dans le sud-est de la Chine au bord dela mer, la province du Fujian s’appelle aussi toutsimplement "Min". Les anc(?)tres d’une grande partie de lapopulation de Taiwan sont venus du Fujian (Min). Les deux

  19. Image du savoir, image du pouvoir dans le Lapidaire

    Directory of Open Access Journals (Sweden)

    Marta LACOMBA

    2007-01-01

    Full Text Available À travers le prologue et les enluminures de présentation, le Lapidaire d’Alphonse X oriente l’interprétation de l’œuvre. Ces paratextes mettent en avant le rôle capital du savoir, représenté par la métaphore du trésor caché, qui a ici une valeur topique. Ils mettent également en exergue le rôle que s’attribue le roi dans la transmission de ce savoir, et placent cette nouvelle attribution royale au cœur de son projet politique.A través del prólogo y las miniaturas de presentación, el Lapidario de Alfonso X orienta la interpretación de la obra. Estos paratextos subrayan el papel capital del saber, representado por la metáfora del tesoro escondido, que tiene aquí un valor tópico. Ponen asimismo de manifiesto el papel que se atribuye el monarca en la transmisión de ese saber y colocan esta nueva atribución real en el centro de su proyecto político.

  20. Aventures radiophoniques du Nouveau Roman

    Directory of Open Access Journals (Sweden)

    Beatrice Nickel

    2015-12-01

    Full Text Available  Aventures radiophoniques du Nouveau Roman Colloque international organisé par l’Université Paul-Valéry Montpellier, en partenariat avec l’Université de Stuttgart 19-20 novembre 2015   Organisateurs :  Pierre-Marie Héron, Annie Pibarot, Université Paul-Valéry Montpellier, centre de recherche Rirra21. Françoise Joly, Beatrice Nickel, Universität Stuttgart 

  1. Du comptoir à la toge

    OpenAIRE

    Buti, Gilbert

    2007-01-01

    Descendant d’une famille de petits notables du Dauphiné, Antoine Anthoine (1749-1826) qui n’a pas pu accéder à la magistrature se destine à la marchandise. Après un apprentissage à Marseille au comptoir des Seimandy, il est nommé, par ces négociants, régisseur pour leur commandite de Constantinople. La mobilisation de sa proche parenté et les soutiens des pouvoirs politiques locaux, nationaux et internationaux lui permettent d’obtenir une mission destinée à ouvrir le commerce de la Russie mér...

  2. Les esclaves du commandant Quiquandon

    OpenAIRE

    Tymowski, Michal

    2003-01-01

    Le 10 janvier 1895, Albert Grodet, gouverneur général du Soudan français, adressa au ministère des Colonies une dépêche accusant le commandant Quiquandon, dirigeant de la région Nord-Est (Ségou), d'exploiter illégalement un domaine sur lequel travaillent 140 esclaves. À partir de ce cas particulier, l'auteur analyse les conflits qui existaient à l'époque entre l'administration civile et un groupe d'officiers soudanais. Il se demande si la possession d'esclaves par des officiers, prenant...

  3. ’Les Baoulé ne sont pas des oiseaux pour manger du riz’. Food, migrations and ecology in South-West Ivory Coast

    Directory of Open Access Journals (Sweden)

    François Ruf

    2010-12-01

    Full Text Available La Côte d’Ivoire est le plus grand théâtre des migrations cacaoyères en Afrique sub-saharienne, depuis le Sahel et les régions de savane vers les forêts humides du golfe de Guinée. Dans tout le sud-ouest de la Côte d’Ivoire, se côtoient trois grands groupes de populations, les autochtones, les migrants d’originaires du centre du pays, et les migrants venus du Burkina Faso, ayant construit des modèles alimentaires spécifiques avant de se rencontrer. L’objectif est d’identifier les évolutions depuis leur rencontre dans les forêts du sud-ouest, puis d’en expliquer les déterminants. Les données collectées auprès de 110 planteurs, par questionnaires et interviews, sont limitées à la composante alimentaire des céréales, tubercules, banane plantain. Le résultat le plus important est une conversion partielle des régimes alimentaires des migrants vers le riz, longtemps l’alimentation de base des autochtones. Au cours de la même période de 30 ans, les autochtones suivent un chemin opposé, réduisant leur consommation de riz, abandonnant presque la production. Pour expliquer cette énigme sociologique, les thèses néo-malthusiennes appliquées à la Côte d’Ivoire, un temps contestées, sont remises à l’ordre du jour, teintées d’innovations boserupiennes. À la croisée des changements écologiques, économiques et sociaux, la raréfaction des terres, la disparition des forêts au cours du déroulement du cycle du cacao, l’accès différencié au travail, jouent un rôle décisif dans ces changements alimentaires, via des bouleversements dans les systèmes de production et les rapports sociaux.The Ivory Coast is the largest space for cocoa migrations in sub-Saharan Africa, extending from the Sahel and savannah regions to the rainforests of the Gulf of Guinea. In the southwest of Ivory Coast, three major population groups live side by side: natives, migrants coming from the central region of the country

  4. Rejets et environnement du CERN

    CERN Document Server

    Vojtyla, P

    2007-01-01

    La radioactivité de l’environnement autour de l’Organisation Européenne pour la Recherche Nucléaire (CERN) et les doses de rayonnements qui en résultent pour la population avoisinante sont contrôlées par la Commission de Sécurité du CERN et de manière indépendante par les autorités compétentes des deux États Hôtes, l’Institut de Radioprotection et de Sûreté Nucléaire (IRSN) côté France et l’Office Fédéral de la Santé Publique (OFSP) côté Suisse (voire Chapitre 8.6). Dans ce rapport, les résultats de mesures concernent en particulier le territoire suisse. L’ensemble des mesures effectuées en 2006 prouve que le fonctionnement des installations du CERN était sans conséquence radiologique sur l’environnement et la population. Le contrôle des émissions montre que les rejets effectifs se situent, également en 2006, nettement en dessous des limites réglementaires. Ce constat est confirmé par le contrôle des immissions dans l’environnement. Le CERN a bien respecté en 2...

  5. Sociologie et sociolinguistique du franbreu

    Directory of Open Access Journals (Sweden)

    Ben-Rafael Eliezer

    2014-07-01

    Full Text Available Des enquêtes ont montré que plus de 20 % des adultes israéliens ont quelque connaissance du français. Parmi cette population, 250 000 à 300 000 personnes pouvaient être considérées comme francophones. Le français a affirmé une présence importante – pas toujours reconnue – dès la phase cruciale du développement de cette société. Une immigration de masse suivit la création de l’État (1948 dont la population a quasiment triplé en moins de deux décennies, avec l’arrivée de plus de 200 000 immigrants d’Afrique du Nord et des dizaines de milliers des Balkans et du Moyen-Orient. Beaucoup parmi ces immigrants étaient francophones – le français étant pour eux soit la première langue soit une deuxième qu’ils contrôlaient. C’est depuis lors que la présence du français est devenue démographiquement significative dans la société israélienne, se prolongeant de nos jours dans l’immigration en provenance de France qui se poursuit jusqu’à aujourd’hui. Comme nous l’avons montré ailleurs (Ben-Rafael et Ben-Rafael 2013, Israël fait l’expérience simultanée de plusieurs francophonies originales qui diffèrent par leurs sources aussi bien que leurs expressions (Ben-Rafael et Ben-Rafael 2013. Un premier modèle est le « français vernaculaire » (voir Boudras-Chapon 2008 amené par les immigrants de classes défavorisées arrivant d’Afrique du nord qui se sont regroupés en Israël. Leur français n’a offert qu’une faible résistance à l’hébreu qui s’est imposée dans le processus d’intégration. Un bilinguisme fonctionnant sur un mode additif au début qui s’est mué progressivement en modèle soustractif. Un second modèle concerne les immigrants de même origine ainsi que des immigrants francophones d’autres pays (pays balkaniques, Turquie ou Egypte formant une strate instruite de classe moyenne, pour qui le français était d’utilisation quotidienne aussi bien que de langue de

  6. Le cas du Haut-Adige ou Tyrol du Sud

    Directory of Open Access Journals (Sweden)

    Licia Bagini Scantamburlo

    2007-06-01

    Full Text Available La situation de cette région italienne est vraiment emblématique des rapports entre « les territoires et l’identité » à cause de la présence de différentes communautés linguistiques autochtones, dont les plus importantes sont les minorités germanophone et latine. S’il est vrai que cette situation existe également dans d’autres régions italiennes, il est incontestable que dans le Haut-Adige/Tyrol du Sud elle présente des caractéristiques très spécifiques et uniques pour l’Italie, car les italo...

  7. De Sumer à Seattle, le voyage du bout du monde

    Directory of Open Access Journals (Sweden)

    Olivier Walther

    2008-12-01

    Full Text Available « Les affaires qui se nouent par-dessus les frontières qui séparent les peuples ne font pas que ces frontières n'existent pas » notait Émile Durkheim en 1895 (1895 : 113. Un peu plus d’un siècle plus tard, l’ouvrage de William J. Bernstein intitulé A Splendid Exchange et sous-titré de manière inspirée How Trade Shaped the World vient apporter une confirmation étayée au sociologue français. De Sumer où fut introduit le commerce du cuivre 3000 ans avant Jésus-Christ, à Seattle où se tint la tr...

  8. COMMUNICATION DU CREDIT AGRICOLE - French version only

    CERN Multimedia

    2003-01-01

    La Direction du Crédit Agricole informe son aimable clientèle du CERN des jours et heures d'ouverture de l'agence du site de Prévessin à compter du mardi 14 janvier 2003 : 1. Horaires pour les opérations bancaires courantes 7 jours sur 7 et 24h/24 avec l'espace libre service bancaire. 2. Horaires conseil du mardi au vendredi - Mardi, de 9h. à 12h. et de 14h.15 à 16h.30. - Mercredi, jeudi et vendredi, de 9h. à 12h. et de 13h.30 à 16h.30. Deux collaboratrices au lieu d'une seront désormais présentes toute la journée du mardi au vendredi pour vous accueillir, vous informer et vous conseiller en crédits et placements (réception conseil sur rendez-vous). Autre nouveauté : les mêmes conseillers seront aussi à votre disposition le samedi, sur notre agence de Gex, de 8h.15 à 13h.05, notamment pour les études de financements habitat. La Direction et toute l'équipe de l'agence du Crédit Agricole vous souhaitent une excellent année 2003.

  9. Approche de prise en charge du trouble du spectre de l’autisme

    Science.gov (United States)

    Lee, Patrick F.; Thomas, Roger E.; Lee, Patricia A.

    2015-01-01

    Résumé Objectif Se pencher sur les critères diagnostiques du trouble du spectre de l’autisme (TSA) comme les définit le Manuel diagnostique et statistique des troubles mentaux, cinquième édition (DSM-V), et concevoir une approche de prise en charge du TSA à l’aide du cadre CanMEDS–Médecine familiale (CanMEDS-MF). Sources d’information Le DSM-V, publié par l’American Psychiatric Association en mai 2013, énonce de nouveaux critères diagnostiques du TSA. Le cadre CanMEDS-MF du Collège des médecins de famille du Canada fournit un plan d’orientation pour la prise en charge complexe du TSA. Nous avons utilisé des données recueillies par le Centers for Disease Control and Prevention afin de déterminer la prévalence du TSA, ainsi que la revue systématique et méta-analyse détaillée effectuée par le National Institute for Health and Care Excellence du R.-U. pour ses lignes directrices sur le TSA dans le but d’évaluer les données probantes issues de plus de 100 interventions. Message principal Selon les données du Centers for Disease Control and Prevention, la prévalence du TSA se chiffrait à 1 sur 88 en 2008 aux États-Unis. La classification du TSA dans la quatrième édition du DSM incluait l’autisme, le syndrome d’Asperger, le trouble envahissant du développement et le trouble désintégratif de l’enfance. La dernière révision du DSM-V réunit tous ces troubles sous la mention TSA, avec différents niveaux de sévérité. La prise en charge du TSA est complexe; elle exige les efforts d’une équipe multidisciplinaire ainsi que des soins continus. Les rôles CanMEDS-MF fournissent un cadre de prise en charge. Conclusion Les médecins de famille sont au cœur de l’équipe de soins multidisciplinaire pour le TSA, et le cadre CanMEDS-MF tient lieu de plan détaillé pour guider la prise en charge d’un enfant atteint de TSA et aider la famille de cet enfant.

  10. An Interpretation of Tevatron SUSY Trilepton Search Results in mSUGRA and in a Model-independent Fashion

    CERN Document Server

    Dube, Sourabh; Somalwar, Sunil; Sood, Alexander

    2008-01-01

    Both the CDF and D0 experiments at the Tevatron search for supersymmetry using the golden three lepton and missing energy "trilepton" signature of chargino-neutralino production. However, the experimental results are presented for specific parameter values of a given model or for custom-made scenarios in the region of sensitivity. By breaking down search sensitivity according to the tau-lepton content of the trileptons, we are able to present in this paper a recipe to extend the interpretation of the Tevatron trilepton search results to the general mSUGRA model. We also attempt to interprete the search results in a model-independent fashion by expressing them in terms of relevant sparticle masses instead of specific parameters of a model such as mSUGRA.

  11. Probing R-parity Violating Interactions via pp-→eμ+X Channel on Tevatron

    Institute of Scientific and Technical Information of China (English)

    SUNYan-Bin; JIANGYi; HUANGJin-Rui; HANLiang; ZHANGRen-You; MAWen-Gan

    2005-01-01

    We investigate the lepton flavor violation processes pp-→eμ+X induced by R-parity violating interactions at the Tevatron hadron collider. The theoretical calculation and Monte Carlo simulation demonstrate that with a set of suitable cuts on experimental observables, one might be capable to reduce the standard model physical background to a controllable level so that the signals of R-parity violating interactions could be detected distinctively. Fbrthermore, clear sneutrino information can be abstracted from the purified event sample where other SUSY scalar quark ""pollution"" is heavily suppressed. We conclude that with a reasonable assumption of 10 fb-1 integrated luminosity, the experiments at the Tevatron machine would have potential to discover sneutrino in the region of mv< 400 GeV via lepton flavor violation eμ production channels, or extend the mass scale constraint up to mv- 550 GeV at 95% CL.

  12. Probing R-parity Violating Interactions via p(p) → eμ + X Channel on Tevatron

    Institute of Scientific and Technical Information of China (English)

    SUN Yan-Bin; JIANG Yi; HUANG Jin-Rui; HAN Liang; ZHANG Ren-You; MA Wen-Gan

    2005-01-01

    We investigate the lepton flavor violation processes p(p) → eμ + X induced by R-parity violating interactions at the Tevatron hadron collider. The theoretical calculation and Monte Carlo simulation demonstrate that with a set of suitable cuts on experimental observables, one might be capable to reduce the standard model physical background to a controllable level so that the signals of R-parity violating interactions could be detected distinctively. Furthermore, clear sneutrino information can be abstracted from the purified event sample where other SUSY scalar quark "pollution" is heavily suppressed. We conclude that with a reasonable assumption of 10 fb-1 integrated luminosity, the experiments at the Tevatron machine would have potential to discover sneutrino in the region of mv(v) ≤ 400 GeV via lepton flavor violation eμ production channels, or extend the mass scale constraint up to mv(v) ≥ 550 GeV at 95% CL.

  13. Wand Z production in association with light and heavy-flavour jets at the LHC and the Tevatron

    Directory of Open Access Journals (Sweden)

    Di Ciaccio Lucia

    2013-11-01

    Full Text Available Recent results on W and Z production in association with light and heavy-flavour jets at the Tevatron and the LHC are reviewed. The integrated luminosity which is used for physics analysis by each of the two Tevatron experiments (CDF and D0 corresponds to a maximum of ≈10 fb−1, at an energy in the centre of massof 1.96 TeV. The LHC analyses of ATLAS and CMS use the data sample collected in 2011 which corresponds to an integrated luminosity of ≈5 fb−1, at an energy in the centre of mass of 7 TeV. Events with W and Z bosons accompanied by jets represent one of the main background samples in the analyses of rare Standard Model processes and in searches for New Physics. Furthermore these measurements provide a test of perturbative QCD calculations and probe the strange and heavy flavour content of the proton.

  14. Measurements of beam halo diffusion and population density in the Tevatron and in the Large Hadron Collider

    CERN Document Server

    Stancari, Giulio

    2014-01-01

    Halo dynamics influences global accelerator performance: beam lifetimes, emittance growth, dynamic aperture, and collimation efficiency. Halo monitoring and control are also critical for the operation of high-power machines. For instance, in the high-luminosity upgrade of the LHC, the energy stored in the beam tails may reach several megajoules. Fast losses can result in superconducting magnet quenches, magnet damage, or even collimator deformation. The need arises to measure the beam halo and to remove it at controllable rates. In the Tevatron and in the LHC, halo population densities and diffusivities were measured with collimator scans by observing the time evolution of losses following small inward or outward collimator steps, under different experimental conditions: with single beams and in collision, and, in the case of the Tevatron, with a hollow electron lens acting on a subset of bunches. After the LHC resumes operations, it is planned to compare measured diffusivities with the known strength of tran...

  15. Yukawa Corrections to Single Top Quark Production at the Fermilab Tevatron in the Two-Higgs-Doublet Models

    CERN Document Server

    Li, C S; Yang, J M; Li, Chong Sheng; Oakes, Robert J.; Yang, Jin Min

    1997-01-01

    We calculate Yukawa corrections of order $\\alpha_{ew} M_t^2/M_W^2$ to s= ingle top quark production via $q \\bar q'\\rightarrow t \\bar b$ at the Fermilab Tevatron in the two-Higgs-doublet models. In our calculation we also keep= the terms proportional to $ M_b^2 \\tan^2 \\beta$ since their effects may becom= e rather important for large $\\tan\\beta$. The corrections can amount to mor= e than a 15\\% reduction in the production cross section relative to the tree lev= el result in the general two-Higgs-doublet model, and a 10\\% enhancement in = the minimal supersymmetric model, which might be observable at a high-luminos= ity Tevatron.

  16. Nouvelles du Centre Aéré de l’Association du Personnel du CERN

    CERN Multimedia

    Jardin d'enfants

    2015-01-01

    Cet été 2015, durant quatre semaines d’été, le Centre Aéré a accueilli plus de 40 enfants âgés de 4 à 6 ans. Devant le succès rencontré, et à la demande des parents, il a été décidé d’en doubler la capacité maximale. A l'été 2016, du 4 au 29 juillet, la structure pourra accueillir les enfants de 4 ans révolus et de moins de 7 ans (nés après le 31/07/2009 mais avant  01/07/2012). Les inscriptions se feront à la semaine durant le mois d'Avril 2016. Les programmes sont en cours d'élaboration cependant nous pouvons déjà vous communiquer le thème conducteur du centre qui sera : à la découverte d'un continent différent chaque ...

  17. Sylvain Fagot, Le cirque. Entre culture du corps et culture du risque

    OpenAIRE

    Crochet-Giacometti, Nicolas

    2011-01-01

    Cet ouvrage écrit par Sylvain Fagot, chercheur en sociologie associé à l'université du Québec, et auteur d'une thèse soutenue en 2003 intitulée « Ethno-sociologie du cirque. Arts de la piste / Arts du corps / Arts du risque », s'intéresse à un monde peu connu : celui du cirque. L'objectif y est de montrer comment chaque forme du cirque, le cirque dit « classique » et le cirque dit « nouveau », ont des stratégies sociales et économiques différentes mais surtout un rapport au corps et au risque...

  18. Study of the neutron strength function and of the diffusion radius as a function of mass number; Etude de la fonction densite de neutron et du rayon de diffusion en fonction du nombre de masse

    Energy Technology Data Exchange (ETDEWEB)

    Morgenstern, J. [Commissariat a l' Energie Atomique, 91 - Saclay (France). Centre d' Etudes Nucleaires

    1968-09-01

    The strength functions S{sub 0} and S{sub 1}, and the scattering length R' are studied. The values of S{sub 0}, S{sub 1} and R' are obtained by shape analysis of the individual resonances observed in total neutron cross-section measurements. These measurements were performed at the Saclay 45 MeV linac by the time of flight method. The best resolution achieved was equal to 0.19 ns/m. We have particularly studied the nuclei around number of mass A = 50, 90, 140 and 200. The experimental values of S{sub 0}, S{sub 1} and R' are compared with optical model calculations. A fairly good agreement is obtained using an optical potential with surface absorption. (author) [French] Nous etudions les fonctions densite S{sub 0} et S{sub 1} ainsi que le rayon de diffusion R'. Les valeurs de S{sub 0}, S{sub 1} et R' sont determinees a partir de l'analyse de forme des resonances individuelles observees lors de la mesure de la section efficace neutronique totale. Cette mesure a ete faite aupres de l'accelerateur lineaire d'electrons de 45 MeV de Saclay par la methode du temps de vol. La meilleure resolution atteinte etait egale a 0.19 ns/m. Nous avons particulierement etudie les noyaux situes vers les nombres de masse A 50, 90, 140 et 200. Nous comparons ensuite les valeurs experimentales de S{sub 0}, S{sub 1} et R' a differents calculs de modele optique. Un bon accord est obtenu avec un potentiel optique a absorption de surface. (auteur)

  19. Combination of Tevatron searches for the standard model Higgs boson in the W+W- decay mode

    NARCIS (Netherlands)

    Aaltonen, T.; et al., [Unknown; Ancu, L.S.; de Jong, S.J.; Filthaut, F.; Galea, C.F.; Hegeman, J.G.; Houben, P.; Meijer, M.M.; Svoisky, P.; van den Berg, P.J.

    2010-01-01

    We combine searches by the CDF and D0 Collaborations for a Higgs boson decaying to W+W-. The data correspond to an integrated total luminosity of 4.8 (CDF) and 5.4 (D0) fb(-1) of p (p) over bar collisions at root s = 1.96 TeV at the Fermilab Tevatron collider. No excess is observed above background

  20. Persistance des épidémies de konzo à Kahemba, République Démocratique du Congo: aspects phénoménologiques et socio-économiques

    Science.gov (United States)

    E-Andjafono, Daniel Okitundu Luwa; Makila-Mabe, Guy Bumoko; Ayanne, Marie-Thérèse Sombo Safi; Kikandau, Jackin Kambale; Mashukano, Nicole; Kayembe, Théodore Kazadi; Ngoyi, Dieudonné Mumba; Boivin, Michael Joseph; Tamfum-Muyembe, Jean-Jacques; Mayambu, Jean-Pierre Banea; Tshala-Katumbay, Désiré

    2014-01-01

    Introduction Identifier les facteurs déterminant la persistance du konzo à Kahemba en République Démocratique du Congo. Méthodes Une enquête transversale a été réalisée à Kahemba en 2011 auprès des ménages de 123 enfants avec konzo (critères OMS) et de 87 enfants sans konzo. La récolte des données s'est faite par interviews, enquête socio-économique par le questionnaire HOME; observation, mesures anthropométriques et examen clinique; mesure du taux de cyanure (CN) dans la farine de manioc et thiocyanate (SCN) urinaire; et analyses sérologiques pour exclure les infections rétrovirales HTLV-I/II et HIV-I/II. L'analyse statistique a été faite par ANOVA, test de Chi-carré, et Kruskall-Wallis au seuil de signification de 0.05. Résultats La survenue et la sévérité du konzo étaient associées à la pauvreté des ménages (p sorcellerie. Conclusion L'intoxication chronique au manioc amer, la malnutrition, ainsi que les croyances superstitieuses favorisent la persistance du konzo à Kahemba. La pauvreté porte le risque d'apparition et de gravité du konzo. Les épidémies de Kahemba dévoilent le risque transgénérationel associé au konzo. L'antécédent de konzo dans la famille élargie constituait un facteur de risque pour la survenue de la maladie (OR= 1,92; p = 0,042). Le taux moyen (±ET) de cyanure dans la farine de manioc était de 92,2 (± 56,2) ppm pour les ménages testés. Les taux moyens (±ET) de SCN urinaire étaient respectivement de 520,4 ± 355,7vs. 382,5± 226,3. PMID:25419339

  1. A search for neutral B meson oscillations at the Tevatron collider experiment DO

    Science.gov (United States)

    Krop, Dan

    We present a search for B0s oscillations using semileptonic Bs → DsmuX (Ds → K0SK ). The data were collected using the DO detector from events produced in s = 1.96 TeV proton-antiproton collisions at the Fermilab Tevatron. The Tevatron is currently the only place in the world that produces B0s mesons and will be until early 2008 when the Large Hadron Collider begins operating at CERN. One of the vital ingredients for the search for B0s oscillations is the determination of the flavor of the B0s candidate ( B0s or B¯0s ) at the time of its production, called initial state flavor tagging. We develop an likelihood based initial state flavor tagger that uses objects on the side of the event opposite to the reconstructed B meson candidate. To improve the performance of this flavor tagger, we have made it multidimensional so that it takes correlations between discriminants into account. This tagging is then certified by applying it to sample of semimuonic B(0,+) decays and measuring the well-known oscillation frequency Deltamd. We obtain Delta md = 0.486 +/- 0.021 ps-1, consistent with the world average. The tagging performance is characterized by the effective efficiency, eD2 = (1.90 +/- 0.41)%. We then turn to the search for B0s oscillations in the above-named channel. A special two-dimensional mass fitting procedure is developed to separate kinematic reflections from signal events. Using this mass fitting procedure in an unbinned likelihood framework, we obtain a 95% C.L. of Deltams > 1.10 ps-1 and a sensitivity of 1.92 ps-1. This result is combined with other analyzed B0s decay channels at DO to obtain a combined 95% C.L. of Delta ms > 14.9 ps.1 and a sensitivity of 16.5 ps-1. The corresponding log likelihood scan has a preferred value of Delta ms = 19 ps-1 with a 90% confidence level interval of 17 < Deltams < 21 ps -1, assuming Gaussian uncertainties. A comparison of the change in the likelihood between Deltams = 19 ps -1 and Deltams = infinity yields an 8

  2. Au croisement des mondialisations. Le cas du chanteur Sami Yusuf At the Crossroads of Globalisation : the Singer Sami Yusuf

    Directory of Open Access Journals (Sweden)

    Farid El Asri

    2011-03-01

    Full Text Available Depuis une dizaine d’années, apparaissent dans le paysage culturel des Musul­mans d’Europe des artistes qui affirment leur foi tout en délivrant un message d’émancipation. Leur art s’articule sur des référents relevant de sphères a priori éloignées. Nous découvrons ainsi des chanteurs dont l’approche artistique est métissée par les interpénétrations des perceptions. Ces “nouvelles stars” s’exportent, au-delà des frontières européennes, au gré du succès qu’ils rem­portent auprès du public. Ainsi, le monde musulman suit-il le parcours de tel ou tel chanteur musulman d’Europe. Le profil de Sami Yusuf est à cet égard para­digmatique. Résidant à Londres, il s’est fait connaître par un style musical qui tente de concilier la tradition du Nasheed, l’éthique langagière et l’esthétique occidentale. Cette relation entre des expressions artistiques locales qui se globalisent nous amène à déconstruire les mécanismes mis en œuvre tant au niveau technique qu’au niveau de l’imaginaire du fan.During the last decennium Muslim artists have emerged in Europe who without renouncing their religion makes for more freedom. Singers, for instance, availing themselves of instruments of dubious orthodoxy, have contributed to the cultural globalization now afoot. These stars are applauded beyond the frontiers of the Old World and their careers are followed eagerly in the Muslim world – Sami Yusuf being typical. Living in London he has combined traditional Nasheed songs with the aesthetic and committed accents of western culture. An analytical understanding of this phenomenon is here proposed.

  3. Chapitre VI. Prudence du financement

    OpenAIRE

    Jambard, Pierre

    2015-01-01

    L’histoire financière de la société permet de comprendre bien des traits de son histoire. Comme toutes les entreprises du bâtiment et des travaux publics, la Société Auxiliaire s’est trouvée devant la nécessité de disposer d’importants capitaux circulants. Grâce à une gestion financière efficace, elle est, en général, parvenue à dégager de son activité les fonds nécessaires, bien que l’aisance de la trésorerie quotidienne n’ait été acquise qu’avec la reconversion. Les années 1927-1946 sont ce...

  4. L’abolition du vieillissement

    Directory of Open Access Journals (Sweden)

    Josef Reindl

    2012-02-01

    Full Text Available I « L’humanité vieillit à un rythme inimaginable. (... »« L’humanité vieillit à un rythme inimaginable. Nous devons résoudre le problème de notre propre vieillissement pour résoudre celui du monde entier. » M. Schirrmacher, l’un des intellectuels médiatiques les plus connus de l’Allemagne, joue comme toujours de façon magistrale la partition de l’effroi. Il ne se contente nullement de s’arranger avec son propre vieillissement, mais il veut sauver le monde à travers « une révolution militante...

  5. DU COTÉ DE CHEZ SOI

    OpenAIRE

    Marc Smeets

    2013-01-01

    Le voyage en Hollande, au XIXe siècle, s'inscrit dans une longue tradition où résonnent les notions de liberté, tolérance et commerce, mais il acquiert aussi une spécificité étant donné l’importance que prend la figure du « chez soi » : les Pays-Bas, terre d'agrément où le voyageur français se sent à l'aise et où il aimerait, si possible, vivre. Proust, de ce point de vue-là, ne fait rien de neuf quand il rêve dans la Recherche d'une « vie domestique » en terre batave. Les Pays-Bas, pour le v...

  6. Sulphite metabolism; Metabolisme du sulfite

    Energy Technology Data Exchange (ETDEWEB)

    Fromageot, P.; Chapeville, F. [Commissariat a l' Energie Atomique, Saclay (France).Centre d' Etudes Nucleaires

    1960-07-01

    Although the formation of sulphite by micro-organisms was observed as early as 1914 by Neuberg, it was only in 1932 that Nightingale showed it to be present inside cells, in the case of tomato leaf stalks, its formation being due to the reaction: SO{sub 3}H{sup -} + (S{sub 2}O{sub 3}){sub 2}{sup --} {yields} S{sub 2}O{sub 3}{sup --} + O{sub 3}S{sub 2}O{sub 3}{sup --}. The presence of the thiosulphate formed was shown by the high refractive index of its barium salt. Today we have a certain amount of data concerning the formation and use of sulphite in the living cell, even through the knowledge is still incomplete. In this article we will describe and discuss the facts which are known, with particular reference to the oxidation of sulphite. (author) [French] Si la formation de sulfite par des micro-organismes a ete observee des 1914 par Neuberg, sa presence a l'interieur des cellules a ete demontree pour la premiere fois par Nightingale en 1932, dans des tiges et des feuilles de tomates, par la reaction: SO{sub 3}H{sup -} + (S{sub 2}O{sub 3}){sub 2}{sup --} {yields} S{sub 2}O{sub 3}{sup --} + O{sub 3}S{sub 2}O{sub 3}{sup --}. Le thiosulfate forme etait mis en evidence par l'indice de refraction eleve de son sel de baryum. Aujourd'hui on possede un certain nombre de donnees, cependant encore tres incompletes, sur la formation du sulfite et son utilisation par la cellule vivante. Dans cet expose nous decrirons et discuterons quelques-unes de ces acquisitions, tout particulierement celles relatives a l'oxydation du sulfite. (auteur)

  7. L’efficacité du conseil d’administration dans les sociétés anonymes au Cameroun: Une lecture par l’hétérogénéité des administrateurs

    Directory of Open Access Journals (Sweden)

    Georges Kriyoss Mfouapon

    2013-12-01

    Full Text Available Le but de cet article est d’analyser l’effet de l’homogénéité ou de l’hétérogénéité du profil des administrateurs sur l’efficacité de leur conseil d’administration (CA. Les données analysées sont collectées auprès de 386 administrateurs répartis sur un échantillon de 64 CA des sociétés anonymes (SA installées au Cameroun. Les résultats obtenus indiquent que l’homogénéité socioprofessionnelle, de l’indépendance et clanique du CA sont d’une influence notable sur leur efficacité. Ces résultats montrent, en fait que, l’hétérogénéité du CA est source d’efficacité supérieure dans les choix stratégiques, et d’inefficacité dans les opérations de contrôle et de surveillance de l’équipe dirigeante. Ces résultats s’inscrivent dans la même perspective que les travaux d’Hambrick & Mason (1984 sur la Upper Echelons Research, la théorie de la régulation clanique d’Ouchi (1980 et constituent en même temps une confirmation des résultats de Jensen (1993.

  8. 8 novembre 2016 - Ambassadeur extraordinaire et plénipotentiaire V. Zellweger, Représentant permanent de la Confédération suisse auprès de l’Office des Nations Unies et des autres organisations internationales à Genève signe le livre d'or en présence de J. Wenninger, C. Warakaulle, F. Gianotti et M. Steinacher.

    CERN Multimedia

    Brice, Maximilien

    2016-01-01

    Son Excellence Monsieur Valentin Zellweger Ambassadeur extraordinaire et plénipotentiaire Représentant permanent de la Confédération Suisse auprès de l’Office des Nations Unies et des autres organisations internationales à Genève Mardi 8 novembre 2016

  9. Inauguration du C/R Forum (Belgique

    Directory of Open Access Journals (Sweden)

    2009-04-01

    Full Text Available Le 16 février dernier, la Vlaamse beroepsvereniging Conservatie en Restauratie Forum (C/R Forum a été constituée à l'initiative de 18 personnes du milieu de la conservation/restauration et du secteur de la protection du patrimoine. Etant donné que la conservation et la gestion du patrimoine culturel mobilier et immobilier de même que la formation et la recherche relèvent des communautés et des régions, la nécessité est apparue depuis un certain temps de créer une organisation Flamande au sei...

  10. Daphne du Maurier' unustatud jutud / Udo Uibo

    Index Scriptorium Estoniae

    Uibo, Udo, 1956-

    2011-01-01

    Ajalehe "The Independent" teatel kavatseb kirjastus "Virago" maikuus avaldada Daphne Du Maurier lühiproosa kogumiku "Nukk" (The Doll), mille on koostanud tema loomingu suur austaja Ann Willmore ja mis sisaldab 13 unustatud ja seni avaldamata novelli

  11. Flaubert et Du Camp : quelques remarques

    Directory of Open Access Journals (Sweden)

    Michel Brix

    2016-12-01

    Full Text Available Les spécialistes de Flaubert ont fait de nombreux reproches à Maxime Du Camp et ne prêtent plus guère d’attention à ce qu’il a écrit. C’est une situation très regrettable, qui prive les lecteurs d’informations nombreuses, susceptibles d’éclairer les enjeux mais aussi les impasses et les contradictions du projet esthétique de Flaubert. Quelques cas significatifs sont évoqués dans le présent article, qui se penche plus particulièrement sur la ressemblance entre un passage du livre de Du Camp Le Nil (1854 et les lignes de L’Éducation sentimentale (1869 qui rapportent l’“apparition” de Mme Arnoux.

  12. Searching for R-Parity Violation at Run II of the Tevatron

    CERN Document Server

    Allanach, Benjamin C; Berger, E L; Chertok, M; De Campos, F; Dedes, A; Díaz, M A; Dreiner, H; Éboli, Oscar J P; Harris, B W; Hewett, J L; Magro, M B; Mondal, N K; Narasimham, V S; Navarro, L; Parua, N; Porod, Werner; Restrepo, D A; Richardson, Peter; Rizzo, T; Seymour, Michael H; Sullivan, Z; Valle, José W F

    1999-01-01

    We present an outlook for possible discovery of supersymmetry with broken R-parity at Run II of the Tevatron. We first present a review of the literature and an update of the experimental bounds. In turn we then discuss the following processes: 1. Resonant slepton production followed by R-parity violating decay, (a) via $LQD^c$ and (b) via $LLE^c$. 2. How to distinguish resonant slepton production from $Z'$ or $W'$ production. 3. Resonant slepton production followed by the decay to neutralino LSP, which decays via $LQD^c$. 4. Resonant stop production followed by the decay to a chargino, which cascades to the neutralino LSP. 5. Gluino pair production followed by the cascade decay to charm squarks which decay directly via $L_1Q_2D^c_1$. 6. Squark pair production followed by the cascade decay to the neutralino LSP which decays via $L_1Q_2D^c_1$. 7. MSSM pair production followed by the cascade decay to the LSP which decays (a) via $LLE^c$, (b) via $LQD^c$, and (c) via $U^cD^cD^c$, respectively. 8. Top quark and t...

  13. First Constraints on SU(5)xU(1) Supergravity from Trilepton Searches at the Tevatron

    CERN Document Server

    López, J L; Park, G T; Wang, X; Zichichi, A

    1993-01-01

    We present the first constraints on the parameter space of $SU(5)\\times U(1)$ supergravity (in both no-scale and dilaton scenarios) which arise from the recently announced limits on trilepton searches at the Tevatron. The trilepton rate has been calculated for those points in parameter space which satisfy not only the minimal theoretical and experimental LEP constraints, but also the {\\em combined} effect of the following indirect experimental constraints: (i) the CLEO limits on the $b\\to s\\gamma$ rate, (ii) the long-standing limit on the anomalous magnetic moment of the muon, (iii) the non-observation of anomalous muon fluxes in underground detectors (``neutrino telescopes"), and (iv) the electroweak LEP high-precision measurements in the form of the $\\epsilon_{1},\\epsilon_b$ parameters. For $m_t=150\\GeV$, the trilepton constraint rules out some regions of parameter space with chargino masses as high as $m_{\\chi^\\pm_1}\\approx105\\GeV$, although it is not possible to establish a new absolute lower bound on the...

  14. Combination of measurements of the top-quark pair production cross section from the Tevatron Collider

    Science.gov (United States)

    Aaltonen, T.; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Agnew, J. P.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J. A.; Arisawa, T.; Artikov, A.; Asaadi, J.; Ashmanskas, W.; Askew, A.; Atkins, S.; Auerbach, B.; Augsten, K.; Aurisano, A.; Avila, C.; Azfar, F.; Badaud, F.; Badgett, W.; Bae, T.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barbaro-Galtieri, A.; Barberis, E.; Baringer, P.; Barnes, V. E.; Barnett, B. A.; Barria, P.; Bartlett, J. F.; Bartos, P.; Bassler, U.; Bauce, M.; Bazterra, V.; Bean, A.; Bedeschi, F.; Begalli, M.; Behari, S.; Bellantoni, L.; Bellettini, G.; Bellinger, J.; Benjamin, D.; Beretvas, A.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bhat, P. C.; Bhatia, S.; Bhatnagar, V.; Bhatti, A.; Bland, K. R.; Blazey, G.; Blessing, S.; Bloom, K.; Blumenfeld, B.; Bocci, A.; Bodek, A.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bortoletto, D.; Boudreau, J.; Boveia, A.; Brandt, A.; Brandt, O.; Brigliadori, L.; Brock, R.; Bromberg, C.; Bross, A.; Brown, D.; Brucken, E.; Bu, X. B.; Budagov, J.; Budd, H. S.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Burkett, K.; Busetto, G.; Bussey, P.; Buszello, C. P.; Butti, P.; Buzatu, A.; Calamba, A.; Camacho-Pérez, E.; Camarda, S.; Campanelli, M.; Canelli, F.; Carls, B.; Carlsmith, D.; Carosi, R.; Carrillo, S.; Casal, B.; Casarsa, M.; Casey, B. C. K.; Castilla-Valdez, H.; Castro, A.; Catastini, P.; Caughron, S.; Cauz, D.; Cavaliere, V.; Cavalli-Sforza, M.; Cerri, A.; Cerrito, L.; Chakrabarti, S.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Chen, Y. C.; Chertok, M.; Chiarelli, G.; Chlachidze, G.; Cho, K.; Cho, S. W.; Choi, S.; Chokheli, D.; Choudhary, B.; Cihangir, S.; Claes, D.; Clark, A.; Clarke, C.; Clutter, J.; Convery, M. E.; Conway, J.; Cooke, M.; Cooper, W. E.; Corbo, M.; Corcoran, M.; Cordelli, M.; Couderc, F.; Cousinou, M.-C.; Cox, C. A.; Cox, D. J.; Cremonesi, M.; Cruz, D.; Cuevas, J.; Culbertson, R.; Cutts, D.; Das, A.; d'Ascenzo, N.; Datta, M.; Davies, G.; de Barbaro, P.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demina, R.; Demortier, L.; Deninno, M.; Denisov, D.; Denisov, S. P.; D'Errico, M.; Desai, S.; Deterre, C.; DeVaughan, K.; Devoto, F.; Di Canto, A.; Di Ruzza, B.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dittmann, J. R.; Dominguez, A.; Donati, S.; D'Onofrio, M.; Dorigo, M.; Driutti, A.; Dubey, A.; Dudko, L. V.; Duperrin, A.; Dutt, S.; Eads, M.; Ebina, K.; Edgar, R.; Edmunds, D.; Elagin, A.; Ellison, J.; Elvira, V. D.; Enari, Y.; Erbacher, R.; Errede, S.; Esham, B.; Evans, H.; Evdokimov, V. N.; Farrington, S.; Feng, L.; Ferbel, T.; Fernández Ramos, J. P.; Fiedler, F.; Field, R.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Flanagan, G.; Forrest, R.; Fortner, M.; Fox, H.; Franklin, M.; Freeman, J. C.; Frisch, H.; Fuess, S.; Funakoshi, Y.; Galloni, C.; Garbincius, P. H.; Garcia-Bellido, A.; García-González, J. A.; Garfinkel, A. F.; Garosi, P.; Gavrilov, V.; Geng, W.; Gerber, C. E.; Gerberich, H.; Gerchtein, E.; Gershtein, Y.; Giagu, S.; Giakoumopoulou, V.; Gibson, K.; Ginsburg, C. M.; Ginther, G.; Giokaris, N.; Giromini, P.; Giurgiu, G.; Glagolev, V.; Glenzinski, D.; Gold, M.; Goldin, D.; Golossanov, A.; Golovanov, G.; Gomez, G.; Gomez-Ceballos, G.; Goncharov, M.; González López, O.; Gorelov, I.; Goshaw, A. T.; Goulianos, K.; Gramellini, E.; Grannis, P. D.; Greder, S.; Greenlee, H.; Grenier, G.; Grinstein, S.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grosso-Pilcher, C.; Group, R. C.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Guimaraes da Costa, J.; Gutierrez, G.; Gutierrez, P.; Hahn, S. R.; Haley, J.; Han, J. Y.; Han, L.; Happacher, F.; Hara, K.; Harder, K.; Hare, M.; Harel, A.; Harr, R. F.; Harrington-Taber, T.; Hatakeyama, K.; Hauptman, J. M.; Hays, C.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinrich, J.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herndon, M.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hocker, A.; Hoeneisen, B.; Hogan, J.; Hohlfeld, M.; Holzbauer, J. L.; Hong, Z.; Hopkins, W.; Hou, S.; Howley, I.; Hubacek, Z.; Hughes, R. E.; Husemann, U.; Hussein, M.; Huston, J.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Introzzi, G.; Iori, M.; Ito, A. S.; Ivanov, A.; Jabeen, S.; Jaffré, M.; James, E.; Jang, D.; Jayasinghe, A.; Jayatilaka, B.; Jeon, E. J.; Jeong, M. S.; Jesik, R.; Jiang, P.; Jindariani, S.; Johns, K.; Johnson, E.; Johnson, M.; Jonckheere, A.; Jones, M.; Jonsson, P.; Joo, K. K.; Joshi, J.; Jun, S. Y.; Jung, A. W.; Junk, T. R.; Juste, A.; Kajfasz, E.; Kambeitz, M.; Kamon, T.; Karchin, P. E.; Karmanov, D.; Kasmi, A.; Kato, Y.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Ketchum, W.; Keung, J.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kilminster, B.; Kim, D. H.; Kim, H. S.; Kim, J. E.; Kim, M. J.; Kim, S. H.; Kim, S. B.; Kim, Y. J.; Kim, Y. K.; Kimura, N.; Kirby, M.; Kiselevich, I.; Knoepfel, K.; Kohli, J. M.; Kondo, K.; Kong, D. J.; Konigsberg, J.; Kotwal, A. V.; Kozelov, A. V.; Kraus, J.; Kreps, M.; Kroll, J.; Kruse, M.; Kuhr, T.; Kumar, A.; Kupco, A.; Kurata, M.; Kurča, T.; Kuzmin, V. A.; Laasanen, A. T.; Lammel, S.; Lammers, S.; Lancaster, M.; Lannon, K.; Latino, G.; Lebrun, P.; Lee, H. S.; Lee, H. S.; Lee, J. S.; Lee, S. W.; Lee, W. M.; Lei, X.; Lellouch, J.; Leo, S.; Leone, S.; Lewis, J. D.; Li, D.; Li, H.; Li, L.; Li, Q. Z.; Lim, J. K.; Limosani, A.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipeles, E.; Lipton, R.; Lister, A.; Liu, H.; Liu, H.; Liu, Q.; Liu, T.; Liu, Y.; Lobodenko, A.; Lockwitz, S.; Loginov, A.; Lokajicek, M.; Lopes de Sa, R.; Lucchesi, D.; Lucà, A.; Lueck, J.; Lujan, P.; Lukens, P.; Luna-Garcia, R.; Lungu, G.; Lyon, A. L.; Lys, J.; Lysak, R.; Maciel, A. K. A.; Madar, R.; Madrak, R.; Maestro, P.; Magaña-Villalba, R.; Malik, S.; Malik, S.; Malyshev, V. L.; Manca, G.; Manousakis-Katsikakis, A.; Mansour, J.; Marchese, L.; Margaroli, F.; Marino, P.; Martínez-Ortega, J.; Martínez, M.; Matera, K.; Mattson, M. E.; Mazzacane, A.; Mazzanti, P.; McCarthy, R.; McGivern, C. L.; McNulty, R.; Mehta, A.; Mehtala, P.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Mesropian, C.; Meyer, A.; Meyer, J.; Miao, T.; Miconi, F.; Mietlicki, D.; Mitra, A.; Miyake, H.; Moed, S.; Moggi, N.; Mondal, N. K.; Moon, C. S.; Moore, R.; Morello, M. J.; Mukherjee, A.; Mulhearn, M.; Muller, Th.; Murat, P.; Mussini, M.; Nachtman, J.; Nagai, Y.; Naganoma, J.; Nagy, E.; Nakano, I.; Napier, A.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Nett, J.; Neu, C.; Neustroev, P.; Nguyen, H. T.; Nigmanov, T.; Nodulman, L.; Noh, S. Y.; Norniella, O.; Nunnemann, T.; Oakes, L.; Oh, S. H.; Oh, Y. D.; Oksuzian, I.; Okusawa, T.; Orava, R.; Orduna, J.; Ortolan, L.; Osman, N.; Osta, J.; Pagliarone, C.; Pal, A.; Palencia, E.; Palni, P.; Papadimitriou, V.; Parashar, N.; Parihar, V.; Park, S. K.; Parker, W.; Partridge, R.; Parua, N.; Patwa, A.; Pauletta, G.; Paulini, M.; Paus, C.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Phillips, T. J.; Piacentino, G.; Pianori, E.; Pilot, J.; Pitts, K.; Plager, C.; Pleier, M.-A.; Podstavkov, V. M.; Pondrom, L.; Popov, A. V.; Poprocki, S.; Potamianos, K.; Pranko, A.; Prewitt, M.; Price, D.; Prokopenko, N.; Prokoshin, F.; Ptohos, F.; Punzi, G.; Qian, J.; Quadt, A.; Quinn, B.; Ranjan, N.; Ratoff, P. N.; Razumov, I.; Redondo Fernández, I.; Renton, P.; Rescigno, M.; Rimondi, F.; Ripp-Baudot, I.; Ristori, L.; Rizatdinova, F.; Robson, A.; Rodriguez, T.; Rolli, S.; Rominsky, M.; Ronzani, M.; Roser, R.; Rosner, J. L.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Ruffini, F.; Ruiz, A.; Russ, J.; Rusu, V.; Sajot, G.; Sakumoto, W. K.; Sakurai, Y.; Sánchez-Hernández, A.; Sanders, M. P.; Santi, L.; Santos, A. S.; Sato, K.; Savage, G.; Saveliev, V.; Savoy-Navarro, A.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schlabach, P.; Schmidt, E. E.; Schwanenberger, C.; Schwarz, T.; Schwienhorst, R.; Scodellaro, L.; Scuri, F.; Seidel, S.; Seiya, Y.; Sekaric, J.; Semenov, A.; Severini, H.; Sforza, F.; Shabalina, E.; Shalhout, S. Z.; Shary, V.; Shaw, S.; Shchukin, A. A.; Shears, T.; Shepard, P. F.; Shimojima, M.; Shochet, M.; Shreyber-Tecker, I.; Simak, V.; Simonenko, A.; Skubic, P.; Slattery, P.; Sliwa, K.; Smirnov, D.; Smith, J. R.; Snider, F. D.; Snow, G. R.; Snow, J.; Snyder, S.; Söldner-Rembold, S.; Song, H.; Sonnenschein, L.; Sorin, V.; Soustruznik, K.; St. Denis, R.; Stancari, M.; Stark, J.; Stentz, D.; Stoyanova, D. A.; Strauss, M.; Strologas, J.; Sudo, Y.; Sukhanov, A.; Suslov, I.; Suter, L.; Svoisky, P.; Takemasa, K.; Takeuchi, Y.; Tang, J.; Tecchio, M.; Teng, P. K.; Thom, J.; Thomson, E.; Thukral, V.; Titov, M.; Toback, D.; Tokar, S.; Tokmenin, V. V.; Tollefson, K.; Tomura, T.; Tonelli, D.; Torre, S.; Torretta, D.; Totaro, P.; Trovato, M.; Tsai, Y.-T.; Tsybychev, D.; Tuchming, B.; Tully, C.; Ukegawa, F.; Uozumi, S.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Van Kooten, R.; van Leeuwen, W. M.; Varelas, N.; Varnes, E. W.; Vasilyev, I. A.; Vázquez, F.; Velev, G.; Vellidis, C.; Verkheev, A. Y.; Vernieri, C.; Vertogradov, L. S.; Verzocchi, M.; Vesterinen, M.; Vidal, M.; Vilanova, D.; Vilar, R.; Vizán, J.; Vogel, M.; Vokac, P.; Volpi, G.; Wagner, P.; Wahl, H. D.; Wallny, R.; Wang, M. H. L. S.; Wang, S. M.; Warchol, J.; Waters, D.; Watts, G.; Wayne, M.; Weichert, J.; Welty-Rieger, L.; Wester, W. C.; Whiteson, D.; Wicklund, A. B.; Wilbur, S.; Williams, H. H.; Williams, M. R. J.; Wilson, G. W.; Wilson, J. S.; Wilson, P.; Winer, B. L.; Wittich, P.; Wobisch, M.; Wolbers, S.; Wolfe, H.; Wood, D. R.; Wright, T.; Wu, X.; Wu, Z.; Wyatt, T. R.; Xie, Y.; Yamada, R.; Yamamoto, K.; Yamato, D.; Yang, S.; Yang, T.; Yang, U. K.; Yang, Y. C.; Yao, W.-M.; Yasuda, T.; Yatsunenko, Y. A.; Ye, W.; Ye, Z.; Yeh, G. P.; Yi, K.; Yin, H.; Yip, K.; Yoh, J.; Yorita, K.; Yoshida, T.; Youn, S. W.; Yu, G. B.; Yu, I.; Yu, J. M.; Zanetti, A. M.; Zeng, Y.; Zennamo, J.; Zhao, T. G.; Zhou, B.; Zhou, C.; Zhu, J.; Zielinski, M.; Zieminska, D.; Zivkovic, L.; Zucchelli, S.; CDF Collaboration

    2014-04-01

    We combine six measurements of the inclusive top-quark pair (tt ¯) production cross section (σtt ¯) from data collected with the CDF and D0 detectors at the Fermilab Tevatron with proton-antiproton collisions at √s =1.96 TeV. The data correspond to integrated luminosities of up to 8.8 fb-1. We obtain a value of σtt ¯=7.60±0.41 pb for a top-quark mass of mt=172.5 GeV. The contributions to the uncertainty are 0.20 pb from statistical sources, 0.29 pb from systematic sources, and 0.21 pb from the uncertainty on the integrated luminosity. The result is in good agreement with the standard model expectation of 7.35-0.33+0.28 pb at next-to-next-to-leading order and next-to-next-to leading logarithms in perturbative QCD.

  15. Inclusive b and b anti b production with quasi-multi-Regge kinematics at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Kniehl, B.A. [Hamburg Univ. (Germany). II. Institut fuer Theoretische Physik; Saleev, V.A.; Shipilova, A.V. [Samara State University (Russian Federation)

    2010-03-15

    We consider b-jet hadroproduction in the quasi-multi-Regge-kinematics approach based on the hypothesis of gluon and quark Reggeization in t-channel exchanges at high energies. The preliminary data on inclusive b-jet and b anti b-dijet production taken by the CDF Collaboration at the Fermilab Tevatron are well described without adjusting parameters. We find the main contribution to inclusive b-jet production to be the scattering of a Reggeized gluon and a Reggeized b-quark to a b quark, which is described by the effective Reggeon-Reggeon-quark vertex. The main contribution to b anti b-pair production arises from the scattering of two Reggeized gluons to a b anti b pair, which is described by the effective Reggeon-Reggeon-quark-quark vertex. Our analysis is based on the Kimber-Martin-Ryskin prescription for unintegrated gluon and quark distribution functions using as input the Martin-Roberts-Stirling-Thorne collinear parton distribution functions of the proton. (orig.)

  16. Heavy octets and Tevatron signals with three or four b jets

    Energy Technology Data Exchange (ETDEWEB)

    Bai, Yang; /SLAC; Dobrescu, Bogdan A.; /Fermilab

    2011-08-12

    Hypothetical color-octet particles of spin 0, pair-produced at hadron colliders through their QCD coupling, may lead to final states involving three or four b jets. We analyze kinematic distributions of the 3b final state that differentiate the scalar octets from supersymmetric Higgs bosons. Studying the scalar sector that breaks an SU(3) x SU(3) gauge symmetry down to the QCD gauge group, we find that the scalar octet is resonantly produced in pairs via a spin-1 octet (coloron). A scalar octet of mass in the 140-150 GeV range can explain the nonstandard shape of the b-jet transverse energy distributions reported by the CDF Collaboration, especially when the coloron mass is slightly above twice the scalar mass. The dominant decay mode of the scalar octet is into a pair of gluons, so that the production of a pair of dijet resonances is large in this model, of about 40 pb at the Tevatron. Even when a W boson is radiated from the initial state, the inclusive cross section for producing a dijet resonance near the scalar octet mass remains sizable, around 0.15 pb.

  17. Probing R-parity violating models of neutrino mass at the Tevatron via top Squark decays

    CERN Document Server

    Das, S P; Guchait, M; Das, Siba Prasad; Datta, Amitava; Guchait, Monoranjan

    2003-01-01

    We have estimated the limiting branching ratio of the R-parity violating (RPV) decay of the lighter top squark, $\\tilde t_1 \\ar l^+ d$ ($l=e$ or $\\mu $ and d is a down type quark of any flavor), as a function of top squark mass($\\MST$) for an observable signal in the di-lepton plus di-jet channel at the Tevatron RUN-II experiment with 2 fb$^{-1}$ luminosity. Our simulations indicate that the lepton number violating nature of the underlying decay dynamics can be confirmed via the reconstruction of $\\MST$. The above decay is interesting in the context of RPV models of neutrino mass where the RPV couplings ($\\lambda'_{i3j}$) driving the above decay are constrained to be small ($\\lsim 10^{-3} - 10^{-4} $). If $\\tilde t_1$ is the next lightest super particle - a theoretically well motivated scenario - then the RPV decay can naturally compete with the R-parity conserving (RPC) modes which also have suppressed widths. The model independent limiting BR can delineate the parameter space in specific supersymmetric mode...

  18. Precision Measurements of Electroweak Parameters with Z Bosons at the Tevatron

    CERN Document Server

    Bodek, Arie

    2015-01-01

    We report on the extraction of $\\sin^2\\theta^{\\rm lept}_{\\rm eff}(M_Z)$ and an indirect measurement of the mass of the W boson from the forward-backward asymmetry of dilepton events in the $Z$ boson mass region at the Tevatron. The data samples of $e^+e^-$ and $\\mu^+\\mu^-$ events collected by the CDF detector correspond to the full 9.4 fb$^{-1}$ run II sample and yield an effective electroweak mixing angle $\\sin^2\\theta^{\\rm lept}_{\\rm eff}(M_Z) = 0.23222 \\pm 0.00046$. The corresponding result reported by the D0 collaboration with the full 9.4 fb$^{-1}$ $e^+e-$ sample is $\\sin^2\\theta^{\\rm lept}_{\\rm eff}(M_Z) = 0.23146 \\pm 0.00047$. The CDF collaboration also extracts the on-shell electroweak mixing angle $ \\sin^2 \\theta_W = 0.22401 \\pm 0.00044$ which corresponds to an indirect measurement of the W boson mass $M_W ({\\rm indirect}) = 80.327 \\pm 0.023 \\;{\\rm GeV}$. The quoted uncertainties include both statistical and systematic contributions.

  19. SVX4 a new deep submicron readout IC for the Tevatron Collider at Fermilab

    CERN Document Server

    Krieger, B; Bacchetta, N; Centro, Sandro; Christofek, L; García-Sciveres, M; Haber, C; Hanagaki, K; Hoff, J; Johnson, M; Von der Lippe, H; Mandelli, E; Meng, G; Nomerotski, A; Pellet, D; Rapidis, P; Utes, M; Walder, J P; Weber, M; Wester, W; Wilkes, T; Yarema, R J; Yao, W; Zimmerman, T

    2004-01-01

    SVX4 is the new silicon strip readout IC designed to meet the increased radiation tolerance requirements for Run IIb at the Tevatron collider. Devices have been fabricated, tested, and approved for production. The SVX4 design is a technology migration of the SVX3D design currently in use by CDF. Whereas SVX3D was fabricated in a 0.8 mu m radiation-hard process, SVX4 was fabricated in a standard 0.25 mu m mixed-signal CMOS technology using the "radiation tolerant by design" transistor topologies devised by the RD-49 collaboration. The specific cell layouts include digital cells developed by the ATLAS Pixel group, and full-custom analog blocks. Unlike its predecessors, the new design also includes the necessary features required for generic use by both the CDF and DO experiments at Fermilab. Performance of the IC includes >20 Mrad total dose tolerance, and ~2000 e- rms equivalent input noise charge with 40 pF input capacitance, when sampled at 132 ns period with an 80 ns preamp risetime. At the nominal digitize...

  20. New Results for Light Gravitinos at Hadron Colliders - Tevatron Limits and LHC Perspectives

    CERN Document Server

    Klasen, M

    2006-01-01

    We derive Feynman rules for the interactions of a single gravitino with (s)quarks and gluons/gluinos from an effective supergravity Lagrangian in non-derivative form and use them to calculate the hadroproduction cross sections and decay widths of single gravitinos. We confirm the results obtained previously with a derivative Lagrangian as well as those obtained with the non-derivative Lagrangian in the high-energy limit and elaborate on the connection between gauge independence and the presence of quartic vertices. We perform extensive numerical studies of branching ratios, total cross sections, and transverse-momentum spectra at the Tevatron and the LHC. From the latest CDF monojet cross section limit, we derive a new and robust exclusion contour in the gravitino-squark/gluino mass plane, implying that gravitinos with masses below 1.3 \\times 10^{-5} to 10^{-8} eV are excluded for squark/gluino-masses below 200 and 1200 GeV, respectively. These limits are complementary to the one obtained by the CDF collabora...

  1. New results for light gravitinos at hadron colliders: Fermilab Tevatron limits and CERN LHC perspectives

    Science.gov (United States)

    Klasen, Michael; Pignol, Guillaume

    2007-06-01

    We derive Feynman rules for the interactions of a single gravitino with (s)quarks and gluons/gluinos from an effective supergravity Lagrangian in nonderivative form and use them to calculate the hadroproduction cross sections and decay widths of single gravitinos. We confirm the results obtained previously with a derivative Lagrangian as well as those obtained with the nonderivative Lagrangian in the high-energy limit and elaborate on the connection between gauge independence and the presence of quartic vertices. We perform extensive numerical studies of branching ratios, total cross sections, and transverse-momentum spectra at the Fermilab Tevatron and the CERN LHC. From the latest CDF monojet cross section limit, we derive a new and robust exclusion contour in the gravitino-squark/gluino mass plane, implying that gravitinos with masses below 2×10-5 to 1×10-5eV are excluded for squark/gluino masses below 200 and 500 GeV, respectively. These limits are complementary to the one obtained by the CDF Collaboration, 1.1×10-5eV, under the assumption of infinitely heavy squarks and gluinos. For the LHC, we conclude that supersymmetric scenarios with light gravitinos will lead to a striking monojet signal very quickly after its startup.

  2. Impact of the A48 collimator on the Tevatron B0 dipoles

    CERN Document Server

    Nicolas, L Y

    2003-01-01

    To protect the CDF detector components in an event of an abort kicker prefire (AKP) in the Tevatron, a new collimator is to be installed at the A48 location during the summer 2003 shutdown. Detailed calculations have shown that this 0.5-m long ''single L-shape'' steel collimator will intercept a bunch of protons when such an incident occurs, providing reliable protection of the CDF main detector at an AKP. It will also mitigate the backgrounds induced by elastic beam-gas interactions upstream of B0. Although the Roman Pot detectors downstream of the A48 collimator will see an increased background, the amount of radiation they will receive either resulting from beam halo interactions in the collimator or during an AKP will not damage their sensitive parts. Secondaries resulting from beam halo interactions with the A48 collimator do not noticeably affect the downstream dipoles. The case of an AKP is quite different. As opposed to halo hits in the ''single-L shape'' unit (around 10 sup 5 p/s), a bunch lost on A4...

  3. A betatron tune fitting package for the Tevatron 21.4 MHz Schottky monitor

    CERN Document Server

    Lebrun, Paul; Todesco, Ezio; You, Jianming; Yuan, Zongwei

    2005-01-01

    Accurate control of the betatron tunes and chromaticities is required to optimize the dynamical aperture of any large synchrotron. The Fermilab Tevatron is equipped with two independent Schottky monitors, one operating at 21.4 MHz and the other 1.7 GHz. While the latter one allows us to characterize individual bunches separated by 396 ns, the former one has a larger Q and can give precise tune measurements. A new front-end and related data acquisition for this 21.4 MHz resonator has been installed and commissioned during the FY04 Collider RunII. Output signal are digitized at 100 KHz. Frequency spectra are transfered to dedicated server nodes and fitted in real time. Such frequency spectra are quite complex, due to inherent noise, horizontal/vertical coupling and synchrotron motion. Sophisticated fitting strategies are required. Optimization of this fitting package on relatively powerful commodity computer allows us to report tune and chromaticity measurements at almost 1 Hz. The architecture of the data acqu...

  4. Search for super symmetry at the Tevatron using the trilepton signature

    Energy Technology Data Exchange (ETDEWEB)

    Dube, Sourabh Shishir [Rutgers Univ., New Brunswick, NJ (United States)

    2008-10-01

    This dissertation describes a search for the associated production of the supersymmetric particles, the chargino and the neutralino, through their R-parity conserving decays to three leptons and missing energy. This search is carried out using the data collected at the CDF experiment at the Tevatron √s = 1.96 TeV p$\\bar{p}$ collider at Fermilab. The results are obtained by combining five independent channels with varying signal to background ratio. Overall, a total of 6.4 ± 1.1 background events from standard model processes and 11.4 ± 1.1 signal events for a particular choice of mSUGRA model parameters are expected. The observation of 7 events in data is consistent with the standard model background expectation, and the mSUGRA model is constrained. Limits are set on the cross section of Chargino-Neutralino pair production, and a limit on the mass of the chargino is extracted. A method of obtaining model-independent results is also discussed.

  5. SVX4: A New Deep-Submicron Readout IC for the Tevatron Collider at Fermilab

    Energy Technology Data Exchange (ETDEWEB)

    Krieger, B.; Alfonsi, S.; Bacchetta, N.; Centro, S.; Christofek, L.; Garcia-Sciveres, M.; Haber, C.; Hanagaki, K.; Hoff, J.; Johnson, M.; vonderLippe, H.; Lujan, P.; Mandelli, E.; Meng, G.; Nomerotski, A.; Pellet, D.; Rapidis, P.; Utes, M.; Walder, J.-P.; Weber, M.; Wester, W.; /LBL, Berkeley /Padua U. /INFN, Padua /Kansas U. /Fermilab /UC,

    2003-10-01

    SVX4 is the new silicon strip readout IC designed to meet the increased radiation tolerance requirements for Run IIb at the Tevatron collider. Devices have been fabricated, tested, and approved for production. The SVX4 design is a technology migration of the SVX3D design currently in use by CDF. Whereas SVX3D was fabricated in a 0.8 {micro}m radiation-hard process, SVX4 was fabricated in a standard 0.25 {micro}m mixed-signal CMOS technology using the ''radiation tolerant by design'' transistor topologies devised by the RD-49 collaboration. The specific cell layouts include digital cells developed by the ATLAS Pixel group, and full-custom analog blocks. Unlike its predecessors, the new design also includes the necessary features required for generic use by both the CDF and D0 experiments at Fermilab. Performance of the IC includes >20 MRad total dose tolerance, and {approx}2000 e-rms equivalent input noise charge with 40 pF input capacitance, when sampled at 132 ns period with an 80 ns preamp risetime. At the nominal digitize/readout rate of 106/53 MHz, the 9 mm x 6.3 mm die dissipates {approx}2 mW/channel average at 2.5 V. A review of typical operation, details of the design conversion process, and performance measurements are covered.

  6. A search for z boson pair production at the Fermilab Tevatron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Jarvis, Chad Ryan [Univ. of Maryland, College Park, MD (United States)

    2007-01-01

    This dissertation describes a search for Z/γ* boson pair production decaying into μμμμ, μμee, and eeee final states with approximately 1 fb-1 of data at the Fermilab Tevatron Collider at √s = 1.96 TeV. The small cross section times branching ratio for each channel mandated a thorough study of the acceptance and efficiencies. After optimization, 1.7 ± 0.1 events are expected for Standard Model production with a background of 0.13 ± 0.03 events. One event was found in the μμee channel. A cross section limit of 4.4 pb is determined at a 95% confidence level for Standard Model production. Additionally, one parameter and two parameter 95% C.L. limits are found for the anomalous neutral trilinear gauge couplings ZZZ* and ZZγ*. The one parameter 95% C.L. coupling limits with a form factor scale of 1.2 TeV are: -0.28 < f$Z\\atop{40}$ < 0.28, -0.31 < f$Z\\atop{50}$ < 0.29, -0.26 < f$γ\\atop{40}$ < 0.26, and -0.30 < f$γ\\atop{50}$ < 0.28.

  7. Precise measurements of the $W$ mass at the Tevatron and indirect constraints on the Higgs mass

    Energy Technology Data Exchange (ETDEWEB)

    Lopes de Sa, Rafael

    2012-04-01

    I describe the latest D0 and CDF W boson mass measurements. The D0 measurement is performed with 4.3 fb{sup -1} of integrated luminosity in the electron decay channel with a data set of 1.68 x 10{sup 8} W candidates. The value of the W boson mass measured by D0 is M{sub W} = 80.375 {+-} 0.023 GeV when combined with the previously analyzed 1 fb{sup -1} of integrated luminosity. The CDF measurement uses 2.2 fb{sup -1} of integrated luminosity in both electron and muon decay channels with a total of 1.1 x 10{sup 8} W candidates. The value of the W boson mass measured by CDF is M{sub W} = 80.387 {+-} 0.019 GeV. I report the combination of these two measurements with previous Tevatron measurements and with the LEP measurements of the W boson mass. The new world average is M{sub W} = 80.385 {+-} 0.015GeV. I discuss the implications of the new measurement to the indirect measurement of the Standard Model Higgs boson mass.

  8. New results on the b^-+c meson at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Rahaman, M.A.; /Pittsburgh U.

    2006-09-01

    The authors present recent results on B{sub c}{sup -} meson from the Tevatron. The B{sub c}{sup -} meson has been observed in semileptonic decays, B{sub c}{sup -} {yields} J/{psi}{ell}{sup -} {nu}X, both by CDF and D0 experiments at a significance larger than 5{sigma}. The D0 experiment has used the candidates in B{sub c}{sup -} {yields} J/{psi}{mu}{sup -} {nu}X decay to extract the mass and lifetime of B{sub c}{sup -} meson. The CDF experiment has used both electron and muon channel candidates in B{sub c}{sup -} {yields} J/{psi}{ell}{sup -} {nu}X decays to measure the relative production times branching ratio with respect to B{sup -} {yields} J/{psi}K{sup -} decay and also measured the lifetime of B{sub c}{sup -} meson in electron channel as {tau}(B{sub c}{sup -}) = 0.463{sub -0.055}{sup +0.073} {+-} 0.036 ps. The CDF experiment has also observed B{sub c}{sup -} {yields} J/{psi}{pi}{sup -} decay with a significance exceeding 6.5{sigma} and has measured the mass of B{sub c}{sup -} meson as M(B{sub c}{sup -}) = 6276.5 {+-} 4.0 {+-} 2.7 MeV/c{sup 2}.

  9. Searching for R-parity violation at run-II of the tevatron.

    Energy Technology Data Exchange (ETDEWEB)

    Allanach, B.; Banerjee, S.; Berger, E. L.; Chertok, M.; Diaz, M. A.; Dreiner, H.; Eboli, O. J. P.; Harris, B. W.; Hewett, J.; Magro, M. B.; Mondal, N. K.; Narasimham, V. S.; Navarro, L.; Parua, N.; Porod, W.; Restrepo, D. A.; Richardson, P.; Rizzo, T.; Seymour, M. H.; Sullivan, Z.; Valle, J. W. F.; de Campos, F.

    1999-06-22

    The authors present an outlook for possible discovery of supersymmetry with broken R-parity at Run II of the Tevatron. They first present a review of the literature and an update of the experimental bounds. In turn they then discuss the following processes: (1) resonant slepton production followed by R{sub P} decay, (a) via LQD{sup c} and (b) via LLE{sup c}; (2) how to distinguish resonant slepton production from Z{prime} or W{prime} production; (3) resonant slepton production followed by the decay to neutralino LSP, which decays via LQD{sup c}; (4) resonant stop production followed by the decay to a chargino, which cascades to the neutralino LSP; (5) gluino pair production followed by the cascade decay to charm squarks which decay directly via L{sub 1}Q{sub 2}D{sub 1}{sup c}; (6) squark pair production followed by the cascade decay to the neutralino LSP which decays via L{sub 1}Q{sub 2}D{sub 1}{sup c}; (7) MSSM pair production followed by the cascade decay to the LSP which decays (a) via LLE{sup c}, (b) via LQD{sup c}, and (c) via U{sup c}D{sup c}D{sup c}, respectively; and (8) top quark and top squark decays in spontaneous R{sub P}.

  10. Search for the Standard Model Higgs Boson in associated production with w boson at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Chun, Xu [Univ. of Michigan, Ann Arbor, MI (United States)

    2009-11-01

    A search for the Standard Model Higgs boson in proton-antiproton collisions with center-of-mass energy 1.96 TeV at the Tevatron is presented in this dissertation. The process of interest is the associated production of W boson and Higgs boson, with the W boson decaying leptonically and the Higgs boson decaying into a pair of bottom quarks. The dataset in the analysis is accumulated by the D0 detector from April 2002 to April 2008 and corresponding to an integrated luminosity of 2.7 fb-1. The events are reconstructed and selected following the criteria of an isolated lepton, missing transverse energy and two jets. The D0 Neural Network b-jet identification algorithm is further used to discriminate b jets from light jets. A multivariate analysis combining Matrix Element and Neural Network methods is explored to improve the Higgs boson signal significance. No evidence of the Higgs boson is observed in this analysis. In consequence, an observed (expected) limit on the ratio of σ (p$\\bar{p}$ → WH) x Br (H → b$\\bar{b}$) to the Standard Model prediction is set to be 6.7 (6.4) at 95% C.L. for the Higgs boson with a mass of 115 GeV.

  11. The Underlying Event in Hard Interactions at the Tevatron pbarp Collider

    CERN Document Server

    Acosta, D; Albrow, M G; Ambrose, D; Amidei, D; Anikeev, K; Antos, J; Apollinari, G; Arisawa, T; Artikov, A; Ashmanskas, W; Azfar, F; Azzi-Bacchetta, P; Bacchetta, N; Bachacou, H; Badgett, W; Barbaro-Galtieri, A; Barnes, V E; Barnett, B A; Baroiant, S; Barone, M; Bauer, G; Bedeschi, F; Behari, S; Belforte, S; Bell, W H; Bellettini, G; Bellinger, J; Benjamin, D; Beretvas, A; Bhatti, A A; Binkley, M; Bisello, D; Bishai, M; Blair, R E; Blocker, C; Bloom, K; Blumenfeld, B; Bocci, A; Bodek, A; Bölla, G; Bolshov, A; Bortoletto, D; Boudreau, J; Bromberg, C; Brubaker, E; Budagov, Yu A; Budd, H S; Burkett, K; Busetto, G; Byrum, K L; Cabrera, S; Campbell, M; Carithers, W; Carlsmith, D; Castro, A; Cauz, D; Cerri, A; Cerrito, L; Chapman, J; Chen, C; Chen, Y C; Chertok, M; Chiarelli, G; Chlachidze, G; Chlebana, F; Chu, M L; Chung, J Y; Chung, W H; Chung, Y S; Ciobanu, C I; Clark, A G; Coca, M; Connolly, A; Convery, M; Conway, J; Cordelli, M; Cranshaw, J; Culbertson, R; Dagenhart, D; D'Auria, S; De Barbaro, P; De Cecco, S; Dell'Agnello, S; Dell'Orso, Mauro; Demers, S; Demortier, L; Deninno, M; De Pedis, D; Derwent, P F; Dionisi, C; Dittmann, J R; Dominguez, A; Donati, S; D'Onofrio, M; Dorigo, T; Eddy, N; Erbacher, R; Errede, D; Errede, S; Eusebi, R; Farrington, S; Feild, R G; Fernández, J P; Ferretti, C; Field, R D; Fiori, I; Flaugher, B; Flores-Castillo, L R; Foster, G W; Franklin, M; Friedman, J; Furic, I; Gallinaro, M; García-Sciveres, M; Garfinkel, A F; Gay, C; Gerdes, D W; Gerstein, E; Giagu, S; Giannetti, P; Giolo, K; Giordani, M; Giromini, P; Glagolev, V; Glenzinski, D; Gold, M; Goldschmidt, N; Goldstein, J; Gómez, G; Goncharov, M; Gorelov, I; Goshaw, A T; Gotra, Yu; Goulianos, K; Gresele, A; Grosso-Pilcher, C; Günther, M; Guimarães da Costa, J; Haber, C; Hahn, S R; Halkiadakis, E; Handler, R; Happacher, F; Hara, K; Harris, R M; Hartmann, F; Hatakeyama, K; Hauser, J; Heinrich, J; Hennecke, M; Herndon, M; Hill, C; Höcker, A; Hoffman, K D; Hou, S; Huffman, B T; Hughes, R; Huston, J; Issever, C; Incandela, J R; Introzzi, G; Iori, M; Ivanov, A; Iwata, Y; Iyutin, B; James, E; Jones, M; Kamon, T; Kang, J; Karagoz-Unel, M; Kartal, S; Kasha, H; Kato, Y; Kennedy, R D; Kephart, R; Kilminster, B; Kim, D H; Kim, H S; Kim, M J; Kim, S B; Kim, S H; Kim, T H; Kim, Y K; Kirby, M; Kirsch, L; Klimenko, S; Koehn, P; Kondo, K; Konigsberg, J; Korn, A J; Korytov, A; Kroll, J; Kruse, M; Krutelyov, V; Kuhlmann, S E; Kuznetsova, N; Laasanen, A T; Lami, S; Lammel, S; Lancaster, J; Lannon, K; Lancaster, M; Lander, R; Lath, A; Latino, G; LeCompte, T; Le, Y; Lee, J; Lee, S W; Leonardo, N; Leone, S; Lewis, J D; Li, K; Lin, C S; Lindgren, M; Liss, T M; Liu, T; Litvintsev, D O; Lockyer, N S; Loginov, A; Loreti, M; Lucchesi, D; Lukens, P; Lyons, L; Lys, J; Madrak, R; Maeshima, K; Maksimovic, P; Malferrari, L; Mangano, Michelangelo L; Manca, G; Mariotti, M; Martin, M; Martin, A; Martin, V; Martínez, M; Mazzanti, P; McFarland, K S; McIntyre, P; Menguzzato, M; Menzione, A; Merkel, P; Mesropian, C; Meyer, A; Miao, T; Miller, R; Miller, J S; Miscetti, S; Mitselmakher, G; Moggi, N; Moore, R; Moulik, T; Mulhearn, M; Mukherjee, A; Müller, T; Munar, A; Murat, P; Nachtman, J; Nahn, S; Nakano, I; Napora, R; Niell, F; Nelson, C; Nelson, T; Neu, C; Neubauer, M S; Newman-Holmes, C; Nigmanov, T; Nodulman, L; Oh, S H; Oh, Y D; Ohsugi, T; Okusawa, T; Orejudos, W; Pagliarone, C; Palmonari, F; Paoletti, R; Papadimitriou, V; Patrick, J; Pauletta, G; Paulini, M; Pauly, T; Paus, C; Pellett, D; Penzo, Aldo L; Phillips, T J; Piacentino, G; Piedra, J; Pitts, K T; Pompos, A; Pondrom, L; Pope, G; Pratt, T; Prokoshin, F; Proudfoot, J; Ptohos, F; Poukhov, O; Punzi, G; Rademacker, J; Rakitine, A; Ratnikov, F; Ray, H; Reichold, A; Renton, P B; Rescigno, M; Rimondi, F; Ristori, L; Robertson, W J; Rodrigo, T; Rolli, S; Rosenson, L; Roser, R; Rossin, R; Rott, C; Roy, A; Ruiz, A; Ryan, D; Safonov, A; Saint-Denis, R; Sakumoto, W K; Saltzberg, D; Sánchez, C; Sansoni, A; Santi, L; Sarkar, S; Savard, P; Savoy-, A; Navarro; Schlabach, P; Schmidt, E E; Schmidt, M P; Schmitt, M; Scodellaro, L; Scribano, A; Sedov, A; Seidel, S; Seiya, Y; Semenov, A; Semeria, F; Shapiro, M D; Shepard, P F; Shibayama, T; Shimojima, M; Shochet, M; Sidoti, A; Sill, A; Sinervo, P; Slaughter, A J; Sliwa, K; Snider, F D; Snihur, R; Spezziga, M; Spinella, F; Spiropulu, M; Spiegel, L; Stefanini, A; Strologas, J; Stuart, D; Sukhanov, A; Sumorok, K; Suzuki, T; Takashima, R; Takikawa, K; Tanaka, M; Tano, V; Tecchio, M; Tesarek, R J; Teng, P K; Terashi, K; Tether, S; Thom, J; Thompson, A S; Thomson, E; Tipton, P; Tkaczyk, S; Toback, D; Tollefson, K; Tonelli, D; Tonnesmann, M; Toyoda, H; Trischuk, W; Tseng, J; Tsybychev, D; Turini, N; Ukegawa, F; Unverhau, T; Vaiciulis, T; Varganov, A; Vataga, E; Vejcik--, S; Velev, G V; Veramendi, G; Vidal, R; Vila, I; Vilar, R; Volobuev, I P; Von der Mey, M; Wagner, R G; Wagner, R L; Wagner, W; Wan, Z; Wang, C; Wang, M J; Wang, S M; Ward, B; Waschke, S; Waters, D; Watts, T; Weber, M; Wester, W C; Whitehouse, B; Wicklund, A B; Wicklund, E; Williams, H H; Wilson, P; Winer, B L; Wolbers, S; Wolter, M; Worm, S; Wu, X; Würthwein, F; Yang, U K; Yao, W; Yeh, G P; Yi, K; Yoh, J; Yoshida, T; Yu, I; Yu, S; Yun, J C; Zanello, L; Zanetti, A; Zetti, F; Zucchelli, S

    2004-01-01

    For comparison of inclusive jet cross sections measured at hadron-hadron colliders to next-to-leading order (NLO) parton-level calculations, the energy deposited in the jet cone by spectator parton interactions must first be subtracted. The assumption made at the Tevatron is that the spectator parton interaction energy is similar to the ambient level measured in minimum bias events. In this paper, we test this assumption by measuring the ambient charged track momentum in events containing large transverse energy jets at $\\sqrt{s}=1800$ GeV and $\\sqrt{s}=630$ GeV and comparing this ambient momentum with that observed both in minimum bias events and with that predicted by two Monte Carlo models. Two cones in $\\eta$--$\\phi$ space are defined, at the same pseudo-rapidity, $\\eta$, as the jet with the highest transverse energy ($E_T^{(1)}$), and at $\\pm 90^o$ in the azimuthal direction, $\\phi$. The total charged track momentum inside each of the two cones is measured. The minimum momentum in the two cones is almost...

  12. Spécificité du terrain en sociologie des arts et de la culture

    Directory of Open Access Journals (Sweden)

    Bruno Péquignot

    2011-04-01

    Full Text Available L’article s’interroge sur la spécificité du terrain en sociologie des arts et de la culture. Il s’agit de montrer que la sur-valorisation sociale de ces activités a des conséquences sur les rapports entre chercheurs et acteurs ou consommateurs d’art et de culture. Activités de distinction sociale, elles provoquent autant de sur-déclaration que de sous-déclaration. Du coté des acteurs, l’intégration de certains discours sociologiques sur les arts fait que les entretiens sont biaisés par une sorte d’hyper-correction savante ; du côté des consommateurs, l’intégration des codes sociaux de distinction, notamment liés à l’école, mais aussi aux médias dominants, impose une échelle de valeur qui écrase certaines pratiques et en souligne d’autres. L’article s’appuie sur quelques exemples d’enquêtes auprès des artistes, comme des consommateurs, pour illustrer cette question.Field specificities for sociology of the arts and cultureIn this article, the author examines the specificities of field studies with regards to the sociology of the arts and culture. It is argued that the over-valorisation of these activities has consequences on the relations between researchers and actors or consumers of art and culture. Constituting activities of social distinction, such activities provoke as many over-declarations as under-declarations. With regards to the actors, the integration of certain sociological views on the arts and culture means that interviews are biased by a sort of scholarly hyper-correction; as for the consummators, the integration of social distinction codes, linked in particular to education but also to dominant expressions, imposes a value scale which crushes certain practices and underlines others. The article uses examples of studies undertaken with artists as well as with consummators to illustrate the argument.La especificidad del espacio propio de la sociología del arte y de la culturaEl autor

  13. Étude socio-terminologique du vocabulaire médical cilubà

    Directory of Open Access Journals (Sweden)

    Emmanuel Kambaja Musampa

    2011-10-01

    Full Text Available

    Abstract: Socioterminological Study of the Ciluba Medical Vocabulary. At the conclusion of an investigation (led by Mbujimayi, in the Democratic Republic of the Congo among medical and paramedical staff who are speakers and users of Ciluba, a Bantu language classified by Guthrie in linguistic zone L31, we have collected, by means of recourse to the docu-mentary evidence, 150 French medical terms translated into Ciluba. These terms have been sub-mitted to a twofold socioterminological analysis: a morphosyntactical and a semantic analysis. It deals with analyzing a medical terminology, still basically conveyed in French. This analysis leads to a morphosyntactic and semantic structure which shows that the medical vocabulary in Ciluba has become general, containing more commonplace terms from classes 7 and 12 than from the other classes. These terms are polysemic, metaphoric, metonymic, synonymic or characterized by synecdoche and semantic shift. Contrary to the established tradition in terminology, monosemy is not the rule. This study deals with African terminology, in this way preparing for a bilingual medi-cal dictionary French–Ciluba.

    Keywords: TERMINOLOGY, GENERAL VOCABULARY, MORPHOSYNTACTIC STRUC-TURE, SEMANTIC STRUCTURE, METAPHOR, POLYSEMY, SYNONYMY, METONOMY, MONOSEMY

    Résumé: À l'issue d'une enquête (menée à Mbujimayi, en République Démocratique du Con-go auprès du personnel médical et paramédical locuteur et utilisateur du cilubà, langue bantoue, classifiée par Guthrie dans la zone linguistique L31, nous avons récolté, grâce au recours préalable au dépouillement documentaire, 150 termes médicaux français traduits en cilubà. Ces termes ont été soumis à une analyse socio-terminologique double: une analyse morphosyntaxique et une ana-lyse sémantique. Il s'agit d'analyser une terminologie médicale, encore essentiellement véhiculée en français. Cette analyse aboutit à une structure morphosyntaxique

  14. La fin du risque zéro : du homegrown jihadism au terrorisme du loup solitaire

    Directory of Open Access Journals (Sweden)

    Rémi Baudouï

    2015-09-01

    Full Text Available Le risque zéro représente un moment historique particulier dans la conceptualisation de la socio-politique du risque. Son application repose au début des années 1980 sur l’hypothèse de la possibilité de progresser dans le domaine de l’anticipation et de la gestion sécuritaire des crises potentielles au point de pouvoir prémunir les populations contre toute forme de menace. Il fut employé dans les domaines de la protection civile et de la sécurité militaire. Comme élément de gouvernance politique, il réfutait l’idée selon laquelle le risque existe en préalable comme catégorie d’acceptabilité collective de la menace.

  15. Aux frontières du politique et du religieux

    Directory of Open Access Journals (Sweden)

    Frédéric Sylvanise

    2006-05-01

    Full Text Available The Autobiography of Miss Jane Pittman met en scène de manière spectaculaire deux figures de leadership noir-américain au XIXe siècle (Ned et au XXe siècle (Jimmy. Ned, fils adoptif de Jane Pittman, se rebaptise Professor Douglass en hommage au leader abolitionniste Frederick Douglass. S’il est fondamentalement laïc (il est instituteur, le texte lui confère néanmoins une dimension religieuse, notamment dans le chapitre intitulé « The Sermon at the River » , qui renvoie à la fois à Moïse (le fleuve et à Jésus (le sermon sur la montagne. Abattu par un tueur à gages, Ned est un martyr dont l’histoire était déjà écrite. Le personnage de Jimmy, attendu par toute une communauté comme le messie (alors que lui aussi est un laïc et un homme qui perd la foi, s’inscrit dans la même histoire. Lettré, éloquent et impliqué dans le mouvement pour les droits civils, il est assassiné comme son prédécesseur. Dans les deux cas, le texte lie donc le politique et le biblique comme s’il ne faisait qu’un : être un leader politique, c’est être un preacher et un messie qui guide le peuple. Il est possible de lire l’évocation de ces deux hommes à la lumière d’une certaine actualité. Ned et Jimmy connaissent en effet un sort proche de celui de Malcolm X et de Martin Luther King, récemment assassinés au moment de l’écriture de The Autobiography of Miss Jane Pittman. C’est l’histoire de la répression du leadership noir, au travers du portrait de deux de ses avatars, qui peut donc se lire en creux ici.

  16. HiggsBounds 2.0.0. Confronting neutral and charged Higgs sector predictions with exclusion bounds from LEP and the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Bechtle, P.; Weiglein, G. [Deutsches Elektronen-Synchrotron (DESY), Hamburg (Germany); Brein, O. [Freiburg Univ. (Germany). Physikalisches Inst.; Heinemeyer, S. [Instituto de Fisica de Cantabria (CSIC-UC), Santander (Spain); Williams, K.E. [Bonn Univ. (Germany). Bethe Center for Theoretical Physics

    2011-03-15

    HiggsBounds 2.0.0 is a computer code which tests both neutral and charged Higgs sectors of arbitrary models against the current exclusion bounds from the Higgs searches at LEP and the Tevatron. As input, it requires a selection of model predictions, such as Higgs masses, branching ratios, effective couplings and total decay widths. HiggsBounds 2.0.0 then uses the expected and observed topological cross section limits from the Higgs searches to determine whether a given parameter scenario of a model is excluded at the 95% C.L. by those searches. Version 2.0.0 represents a significant extension of the code since its first release (1.0.0). It includes now 28/53 LEP/Tevatron Higgs search analyses, compared to the 11/22 in the first release, of which many of the ones from the Tevatron are replaced by updates. As a major extension, the code allows now the predictions for (singly) charged Higgs bosons to be confronted with LEP and Tevatron searches. Furthermore, the newly included analyses contain LEP searches for neutral Higgs bosons (H) decaying invisibly or into (non flavour tagged) hadrons as well as decay-mode independent searches for neutral Higgs bosons, LEP searches via the production modes {tau}{sup +}{tau}{sup -}H and b anti bH, and Tevatron searches via t anti tH. Also, all Tevatron results presented at the ICHEP'10 are included in version 2.0.0. As physics applications of HiggsBounds 2.0.0 we study the allowed Higgs mass range for model scenarios with invisible Higgs decays and we obtain exclusion results for the scalar sector of the Randall-Sundrum model using up-to-date LEP and Tevatron direct search results. (orig.)

  17. Search for charginos and neutralinos in the like sign dimuon channel with the D0-FNAL experiment; Recherche de charginos et neutralinos dans le canal dimuon de meme signe aupres de l'experience D0-FNAL

    Energy Technology Data Exchange (ETDEWEB)

    Lesne, V

    2006-07-15

    In the framework of the mSUGRA model which provides a simple breaking mechanism of supersymmetry, sparticles with masses beyond the kinematic reach of the LEP-II experiments may be produced at the Tevatron pp-bar collider at a center of mass energy of 1.96 TeV. A promising source of sparticles at the Tevatron collider is the associated production of the lightest chargino, {chi}-tilde{sub 1}{sup {+-}}, and the next to lightest neutralino, {chi}-tilde{sub 2}{sup 0}. Leptonic decay modes, {chi}-tilde{sub 2}{sup 0} {yields} {chi}-tilde{sub 1}{sup 0}l{sup +}l{sup -} and {chi}-tilde{sub 1}{sup {+-}}l{sup {+-}}{nu}{sub l}, lead to a clean detector signature with three leptons and a large amount of missing transverse energy. In order to increase the sensitivity to signal in regions of mSUGRA parameters space leading to a very soft third lepton with small reconstruction efficiency, a selection based on 2 like sign leptons plus missing transverse energy has been developed. The particular signature with 2 like sign muons is presented in this work. No evidence for supersymmetry has been observed in a dataset collected from April 2002 to February 2006 with the D0 detector at the Tevatron collider and corresponding to an integrated luminosity of 0.9 fb{sup -1}. Then, limits on the product of the cross-section and the 3-leptonic branching ratio, {sigma}(pp-bar {yields} {chi}-tilde{sub 1}{sup {+-}}{chi}-tilde{sub 2}{sup 0}) * BR(3l), have been set as a function of the {chi}-tilde{sub 1}{sup {+-}} mass. The results obtained with the like sign dimuon selection have been combined with the results of three tri-lepton selections. For mSUGRA models with enhanced leptonic decays, a {chi}-tilde{sub 1}{sup {+-}} mass limit of 140 GeV/c{sup 2} has been derived at 95% confidence level. (author)

  18. Mesure de la masse du quark top dans le canal dileptonique électron-muon avec la méthode des éléments de matrice dans l'expérience ATLAS auprès du LHC

    CERN Document Server

    Demilly, Aurélien; Beau, Tristan

    The LHC produced proton-proton collisions data at 7 TeV of center of mass energy in 2011 and 8 TeV in 2012, corresponding to integrated luminosity of, respectively, 5 fb$^{-1}$ and 23 fb$^{-1}$. Data acquired by ATLAS have led to a better understanding of the detector and its performance, to many measurements of physical quantities and the discovery of the Higgs boson. Top quark is involved in many processes beyond the Standard Model. Its mass is an important parameter for the Standard Model and any New Physics theory, thus precisely measuring its mass is necessary. After a description of the Standard Model of Particle Physics, and the role of the top quark in it, the first half of this thesis describes the ATLAS detector and it electromagnetic calorimeter, for which a study of the calibration constant patching is detailed. The second half details top quark physics events detected in ATLAS and their selection. Theoretical aspects of the matrix element method and its implementation for the top quark mass measu...

  19. Analyse du canal $B^0 _s \\to J/\\psi {\\overline{k}}^{*0}$ et contraintes sur les processus pingouins dans les désintégrations $B^0 _s \\to J/\\psi\\phi$ auprès du détecteur LHCb

    CERN Document Server

    AUTHOR|(CDS)2084546

    Within the Standard Model, the decay $B^0_s\\to J/\\psi \\phi$, can occur via two main processes: the predominant tree and the sub-leading penguin. Penguin contributions have been so far ignored. Controlling them is crucial in order to disentangle Standard Model effects from possible New Physics in the measurement of $\\phi_s$. We studied the $B^0_s\\to J / \\psi

  20. Study of production associated to the Higgs boson, HW, Ht t-bar, HZ {yields} {gamma}{gamma} + e{sup {+-}}/{mu}{sup {+-}} + X with the ATLAS detector at LHC; Etude de la production associee du boson de Higgs HW, Htt-bar, HZ {yields} {gamma}{gamma} + e{sup {+-}}/{mu}{sup {+-}} + X avec le detecteur ATLAS, aupres du LHC

    Energy Technology Data Exchange (ETDEWEB)

    Eynard, Guillaume [Laboratoire d`Annecy-le-Vieux de Physique des particules, Grenoble-1 Univ., 74 Annecy (France)

    1998-05-06

    The quest for the Higgs boson, sign of the electromagnetic symmetry breaking, is the main purpose of the ATLAS detector, which will be placed on LHC, the next proton collider scheduled for the year 2005. In this thesis, the liquid argon electromagnet calorimeter, with its special accordion geometry, is used. First, a new method has been implemented for the electronics calibration. Based on the optimal filtering method, wights set used to reconstruct the calibration signal amplitude is computed in a direct way, including non-linearity corrections. Secondly, the electromagnetic calorimeter has been used to evaluate the observability of the Standard Model Higgs boson in the associated production channel: for a mass ranging from 80 to 120 GeV, it decays into two photons and is produced in association with a W or Z boson, or top quark pair, decaying into electrons or muons. Compared to inclusive channel, this charged lepton helps in finding interaction vertex to improve photon-photon mass resolution. Signal and numerous reducible and irreducible backgrounds have been simulated. Selection criteria have been optimized to maximize the number of signal events compared to background ones. This study allows to confirm the observability of the Standard Model Higgs boson in the associated production channel. Moreover, in the MSSM framework, it allows to expand (M{sub A}; tan{beta}) parameter space covering, in the region of low tan{beta} values, towards low M{sub A} values, compared to inclusive channel 50 refs., 76 figs., 48 tabs.

  1. Performance of the Alice muon spectrometer. Weak boson production and measurement in heavy-ion collisions at LHC; Performance du spectrometre a muons d'ALICE. Production et mesure des bosons faibles dans des collisions d'ions lourds aupres du LHC

    Energy Technology Data Exchange (ETDEWEB)

    Conesa del valle, Z

    2007-07-15

    Lattice QCD predicts a transition from a hadronic phase to a Quark Gluon Plasma phase, QGP, for temperatures above 10{sup 13} K. Heavy-ion collisions are proposed to recreate it in laboratory. With such a purpose, the LHC (Large Hadron Collider) will provide Pb-Pb collisions at 5.5 TeV/u, and the ALICE experiment will permit to explore them. In particular, the ALICE muon spectrometer will permit to investigate the muon related probes (quarkonia, open beauty,...). The expected apparatus performances to measure muons and dimuons are discussed. A factorization technique is employed to unravel the different contributions to the global efficiency. Results indicate that the detector should be able to measure muons up to pT {approx} 100 GeV/c with a resolution of about 10 per cent. We show that weak bosons production could be measured for the first time in heavy-ion collisions. Single muon p{sub T} and dimuons invariant mass distributions will probe W and Z production. As mainly muons from b- and c-quarks decays will populate the intermediate-p{sub T} of 5 - 25 GeV/c, heavy quark in-medium energy loss calculations indicate that the single muon spectra would be suppressed by a factor 2-4 in the most central 0 - 10% Pb-Pb collisions at 5.5 TeV. However, for p{sub T} > 35 GeV/c the weak boson decays are predominant, and no suppression is expected. Estimations indicate that the b- and W-muons crossing point shifts down in transverse momenta by 5 to 7 GeV/c in the most central 0 - 10% Pb-Pb collisions at 5.5 TeV. (author)

  2. Comportement du carbone aux joints de grains du molybdène

    OpenAIRE

    1994-01-01

    Pas de résumé en anglais; La mise en évidence et l'interprétation du rôle bénéfique du carbone et du rôle néfaste de l'oxygène sur la cohésion intergranulaire du molybdène en l'absence de précipitation visible au MEB constituaient le but de cette étude. Une méthode efficace de purification du molybdène a été mise au point. Les mesures de la concentration intergranulaire de carbone en fonction de la température de carburation et de la teneur volumique ont été effectuées à l'aide d'un spectromè...

  3. DU COTÉ DE CHEZ SOI

    Directory of Open Access Journals (Sweden)

    Marc Smeets

    2013-12-01

    Full Text Available Le voyage en Hollande, au XIXe siècle, s'inscrit dans une longue tradition où résonnent les notions de liberté, tolérance et commerce, mais il acquiert aussi une spécificité étant donné l’importance que prend la figure du « chez soi » : les Pays-Bas, terre d'agrément où le voyageur français se sent à l'aise et où il aimerait, si possible, vivre. Proust, de ce point de vue-là, ne fait rien de neuf quand il rêve dans la Recherche d'une « vie domestique » en terre batave. Les Pays-Bas, pour le voyageur français au XIXe, c'est le home sweet home.

  4. HiggsSignals. Confronting arbitrary Higgs sectors with measurements at the Tevatron and the LHC

    Energy Technology Data Exchange (ETDEWEB)

    Bechtle, Philip [Bonn Univ. (Germany). Physikalisches Inst.; Heinemeyer, Sven [Instituto de Fisica de Cantabria (CSIC-UC), Santander (Spain); Staal, Oscar [Stockholm Univ. (Sweden). The Oskar Klein Centre; Stefaniak, Tim [Bonn Univ. (Germany). Physikalisches Inst.; Bonn Univ. (Germany). Bethe Center for Theoretical Physics; Weiglein, Georg [Deutsches Elektronen-Synchrotron (DESY), Hamburg (Germany)

    2013-05-15

    HiggsSignals is a Fortran90 computer code that allows to test the compatibility of Higgs sector predictions against Higgs rates and masses measured at the LHC or the Tevatron. Arbitrary models with any number of Higgs bosons can be investigated using a model-independent input scheme based on HiggsBounds. The test is based on the calculation of a {chi}{sup 2} measure from the predictions and the measured Higgs rates and masses, with the ability of fully taking into account systematics and correlations for the signal rate predictions, luminosity and Higgs mass predictions. It features two complementary methods for the test. First, the peak-centered method, in which each observable is defined by a Higgs signal rate measured at a specific hypothetical Higgs mass, corresponding to a tentative Higgs signal. Second, the mass-centered method, where the test is evaluated by comparing the signal rate measurement to the theory prediction at the Higgs mass predicted by the model. The program allows for the simultaneous use of both methods, which is useful in testing models with multiple Higgs bosons. The code automatically combines the signal rates of multiple Higgs bosons if their signals cannot be resolved by the experimental analysis. We compare results obtained with HiggsSignals to official ATLAS and CMS results for various examples of Higgs property determinations and find very good agreement. A few examples of HiggsSignals applications are provided, going beyond the scenarios investigated by the LHC collaborations. For models with more than one Higgs boson we recommend to use HiggsSignals and HiggsBounds in parallel to exploit the full constraining power of Higgs search exclusion limits and the measurements of the signal seen at m{sub H} {approx} 125.5 GeV.

  5. Séroprévalence des marqueurs viraux sur les dons du sang au Centre de Transfusion Sanguine, Hôpital Militaire d’Instruction Mohammed V de Rabat

    Science.gov (United States)

    Uwingabiye, Jean; Zahid, Hafidi; Unyendje, Loubet; Hadef, Rachid

    2016-01-01

    Le but de ce travail était de déterminer la prévalence du virus de l’immunodéficience humaine (VIH), du virus de l’hépatite B (VHB) et C (VHC) sur les dons du sang collectés au Centre de transfusion sanguine(CTS) de l’hôpital militaire d’instruction Mohammed V entre 2010 et 2012. Etude rétrospective menée auprès des donneurs de sang militaires âgés de 18 à 50 ans avec prédominance masculine (95%). L’entretien médical pré-don constitue la première barrière de sélection des sujets à risque. Le dépistage biologique était réalisé par technique immuno-enzymatique en milieu liquide utilisant des anticorps et/ou des antigènes. L’ELISA (enzyme linked immuno-sorbent assay) combiné de quatrième génération pour VHC et VIH a été utilisé. La confirmation a été faite en réalisant la même technique en double au CTS et au laboratoire de virologie. Dans notre série de 25661 échantillons testés, la prévalence du VHB était 3,97‰ (n=102), celle de VHC était 2,45 ‰ (n=63), celle de VIH était 0,15 ‰ (n=4). Un seul cas de coïnfection (0,039 ‰) par le VHB et VHC a été noté, aucune association entre VIH-VHB, VIH-VHC ou VHB, VHC et VIH n’a été enregistrée. Les taux faibles de séroprévalence des marqueurs viraux de notre étude montrent l’amélioration des mesures préventives en ce qui concerne la sélection des donneurs et des tests de dépistage. Cette prévalence constatée incite à maintenir l’utilisation du réactif combiné qui est la seule alternative à la biologie moléculaire pour les pays en voie de développement. PMID:28292147

  6. Temps professionnel et temps personnel des travailleuses du care : perméabilité ou clivage ? Care Workers’ professional time and personal time: permeability or disconnection? The hazard of the “right distance”

    Directory of Open Access Journals (Sweden)

    Pascale Molinier

    2009-09-01

    Full Text Available Les recherches en ergonomie ont montré de longue date l’existence d’une perméabilité psychologique entre les temps professionnels et personnels. Toutefois la situation des travailleuses du care a peu été étudiée sous cet angle. Les femmes qui ont à faire avec les mêmes sortes d’activités, au travail et à domicile, seraient-elles plus vulnérables que d’autres et plus susceptibles de connaître un surmenage ? L’article traite de cette question à partir d’enquêtes de psychodynamique du travail réalisées auprès d’infirmières. Pour les infirmières ayant elles-mêmes des enfants, la confrontation professionnelle avec la maladie et la mort d’enfants est particulièrement anxiogène. Différentes conduites défensives sont décrites et analysées : les stratégies de distanciation affective, de cloisonnement temporel, l’activisme et l’intolérance à la plainte de ses propres enfants. Ces stratégies protectrices visent à instaurer un clivage entre vies professionnelle et privée. Ce clivage est en partie inévitable, mais il augmente en importance, au prix d’une perte du sens du travail, quand les conditions qui autorisent le libre jeu du collectif comme instance d’élaboration de la souffrance dans le travail sont dégradées.Ergonomic research has long shown that professional and personal times are permeable. Yet, the situation of care workers has seldom been studied from that point of view. Are women who have to cope with the same activities both at work and at home more vulnerable than others? more likely to experience burnout? The author tackles the question, beginning with psychodynamic investigations on nurses. For nurses who are mothers themselves, coping with the illness and death of children is particularly anxiety-ridden. Various defensive behaviours are described and analyzed: remaining emotionally aloof, separating time periods, being militant, finding one’s own children’s complaints

  7. Cirque du Monde as a health intervention

    Science.gov (United States)

    Fournier, Cynthia; Drouin, Mélodie-Anne; Marcoux, Jérémie; Garel, Patricia; Bochud, Emmanuel; Théberge, Julie; Aubertin, Patrice; Favreau, Gil; Fleet, Richard

    2014-01-01

    Abstract Objective To present Cirque du Soleil’s social circus program, Cirque du Monde, to explore its potential as a primary health care tool for family physicians. Data sources A review of the literature in PubMed, the Cochrane Library, PsycINFO, LaPresse, Eureka, Google Scholar, and Érudit using the key words circus, social circus, Cirque du Monde, and Cirque du Soleil; a Montreal-based initiative, Espace Transition, modeled on Cirque du Monde; and personal communication with Cirque du Soleil’s Social Circus Training Advisor. Study selection The first 50 articles or websites identified for each key word in each of the databases were examined on the basis of their titles and abstracts in the case of articles, and on the basis of their titles and page content in the case of websites. Articles and websites that explored an aspect of social circuses or that described an intervention that involved circuses were then retained for analysis. Because all literature on social circuses was searched, no criterion for year of publication was used. Synthesis No articles on the social circus as a health intervention were found. One study on the use of the circus as an intervention in schools was identified. It demonstrated an increase in self-esteem in the children who took part. One study on the use of the circus in a First Nations community was found; it contained nonspecific, qualitative findings. The other articles identified were merely descriptions of social circuses. One website was identified on the use of the social circus to help youth who had been treated in a hospital setting for major psychiatric disorders to re-enter the community. The team in the pediatric psychiatry department at Centre Hospitalier Universitaire Sainte-Justine, the children’s hospital in Montreal, Que, was contacted; they were leading this project, called Espace Transition. The unpublished preliminary findings of its pilot project demonstrate substantial improvements in overall patient

  8. Influence du pH, d'acides aminés et de diverses substances organiques sur la fongitoxicité du pyriméthanil, du glufosinate, du captafol, du cymoxanil et du fenpiclonil vis-à-vis de certaines souches de Botrytis cinerea

    OpenAIRE

    1994-01-01

    L’effet du pyriméthanil, du fenpiclonil, du captafol, du glufosinate et du cymoxanil sur l’élongation des filaments germinatifs des spores de Botrytis cinerea est étudié dans diverses conditions culturales du champignon. Si le fenpiclonil présente un niveau d’activité stable entre pH 3,6 et 7,3, en revanche les autres pesticides voient leur toxicité chuter dans des milieux acides (ex pyriméthanil) ou neutres à faiblement basiques (ex captafol, cymoxanil, glufosinate). L’adjonction d’extrait d...

  9. L’internationalisation du roman arabe

    Directory of Open Access Journals (Sweden)

    Dr Dalia Khraibani

    2016-09-01

    Full Text Available La littérature arabe est presque invisible dans l’espace littéraire mondiale pour des raisons diverses. Pourtant, des écrivains réussissent à s’imposer sur la scène littéraire internationale et leurs œuvres deviennent des chefs d’œuvre de la littérature mondiale. Parmi ces écrivains, nous citons Tayeb Saleh qui connaît un succès international surtout avec la parution de son second roman "Saison de migration vers le Nord". Notre étude vise à montrer comment ce roman par son contenu et sa forme, occupe une place de choix dans la littérature mondiale. En effet, nous allons examiner le contexte historique de l’émergence du roman qui joue un rôle dans sa diffusion au niveau mondial. L’une des clés de réussite du roman est la technique narrative qui retient l’haleine du lecteur dès la première page. De plus, le roman répond à l’horizon d’attente du lectorat occidental en représentant des images particulières de la société arabo-africaine qui correspondent aux stéréotypes et clichés du public occidental vis-à-vis des Arabes.

  10. Établissements recevant du public

    CERN Document Server

    2014-01-01

    Synthèse pour les installations électriques, des règles de sécurité contre les risques d’incendie et de panique dans les établissements recevant du public (ERP), selon l’arrêté du 25 juin 1980 modifié. L'ouvrage traite à la fois des dispositions communes aux établissements du 1er groupe (1ère à 4ème catégorie), du 2ème groupe (5ème catégorie) et des règles particulières applicables aux différents types d'établissements (structures d'accueil pour personnes âgées ou handicapées, hôtels, magasins de vente, restaurants et débit de boisson, établissements de soins, administration, châpiteaux, etc...) Sont ainsi notamment traités, dans le cadre des dispositions communes aux établissements du 1er groupe, pour les installations électriques normales : les installations des appareils, tableaux et canalisations, les locaux électriques et installation de machines, l'éclairage normal des locaux accessibles au public, le chauffage et la ventilation, l'installation d'eau chaude sanita...

  11. De Gainsborough à Turner : l'âge d'or du paysage et du portrait anglais dans les collections du musée du Louvre

    OpenAIRE

    Adrien, Muriel

    2015-01-01

    L’exposition De Gainsborough à Turner : l'âge d'or du paysage et du portrait anglais dans les collections du musée du Louvre co-organisée par le Musée du Louvre, le Musée d’Art et d’Archéologie de Valence et le Musée des Beaux-arts de Quimper présentait une sélection de 35 peintures de la collection du Louvre, complétée par 38 dessins du département des Arts Graphiques. Les commissaires de l'exposition étaient : Guillaume Faroult, conservateur en charge des peintures françaises du 18ème siècl...

  12. Search for beyond standard model physics (non-SUSY) in final states with photons at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Palencia, Jose Enrique; /Fermilab

    2009-01-01

    We present the results of searches for non-standard model phenomena in photon final states. These searches use data from integrated luminosities of {approx} 1-4 fb{sup -1} of p{bar p} collisions at {radical}s = 1.96 TeV, collected with the CDF and D0 detectors at the Fermilab Tevatron. No significant excess in data has been observed. We report limits on the parameters of several BSM models (excluding SUSY) for events containing photons.

  13. The Higgs boson in the Standard Model theoretical constraints and a direct search in the wh channel at the Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Huske, Nils Kristian [Pierre and Marie Curie Univ., Paris (France); Bielefeld Univ. (Germany)

    2010-09-10

    We have presented results in two different yet strongly linked aspects of Higgs boson physics. We have learned about the importance of the Higgs boson for the fate of the Standard Model, being either only a theory limited to explaining phenomena at the electroweak scale or, if the Higgs boson lies within a mass range of 130 < mH < 160 GeV the SM would remain a self consistent theory up to highest energy scales O(mPl). This could have direct implications on theories of cosmological inflation using the Higgs boson as the particle giving rise to inflation in the very early Universe, if it couples non-minimally to gravity, an effect that would only become significant at very high energies. After understanding the immense meaning of proving whether the Higgs boson exists and if so, at which mass, we have presented a direct search for a Higgs boson in associated production with a W boson in a mass range 100 < mH < 150 GeV. A light Higgs boson is favored regarding constraints from electroweak precision measurements. As a single analysis is not yet sensitive for an observation of the Higgs boson using 5.3 fb-1 of Tevatron data, we set limits on the production cross section times branching ratio. At the Tevatron, however, we are able to combine the sensitivity of our analyses not only across channels or analyses at a single experiment but also across both experiments, namely CDF and D0. This yields to the so-called Tevatron Higgs combination which, in total, combines 129 analyses from both experiments with luminosities of up to 6.7 fb-1. The results of a previous Tevatron combination led to the first exclusion of possible Higgs boson masses since the LEP exclusion in 2001. The latest Tevatron combination from July 2010 can be seen in Fig. 111 and limits compared to the Standard Model expectation are listed in Table 23. It excludes a SM Higgs boson in the regions of 100 < mH < 109 GeV as well as 158 < m

  14. Inverse muon decay,. nu. sub. mu. +e yields. mu. sup - +. nu. sub e , at the Fermilab Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Mishra, S.R.; Bachmann, K.T.; Blair, R.E.; Foudas, C.; King, B.J.; Lefmann, W.C.; Leung, W.C.; Oltman, E.; Quintas, P.Z.; Rabinowitz, S.A.; Sciulli, F.J.; Seligman, B.; Shaevitz, M.H.; Smith, W.H. (Columbia Univ., New York (USA)); Merritt, F.S.; Oreglia, M.J.; Schumm, B.A. (Chicago Univ., IL (USA)); Bernstein, R.H.; Borcherding, F.; Fisk, H.E.; Lamm, M.J.; Marsh, W.; Merritt, K.W.B.; Schellman, H.; Yovanovitch, D.D. (Fermi National Accelerator Lab., Batavia, IL (USA)); Bodek, A.; Budd, H.S.; De Barbaro, P.; Sakumoto, W.K. (Rochester Univ., NY (USA))

    1990-12-06

    We report an improved measurement of the inverse muon decay process, v{sub {mu}}+e{yields}{mu}{sup -}+v{sub e}, at the Fermilab Tevatron. The rate of this reaction with respect to the v{sub {mu}}-N charged current interaction is measured to be (0.1245{plus minus}0.0057(stat.){plus minus}0.0031(sys.))x10{sup -2}. The measurement confirms the standard model predictions for the Lorentz structure of the weak current, the helicity of the neutrino, and the energy dependence of the cross section. (orig.).

  15. Combination of Tevatron searches for the standard model Higgs boson in the W+W- decay mode

    Energy Technology Data Exchange (ETDEWEB)

    Aaltonen, T.; Abazov, V.M.; Gregores, E.M.; Mercadante, P.G.; /ABC Federal U.; Hebbeker, T.; Kirsch, M.; Meyer, A.; Sonnenschein, L.; /Aachen, Tech. Hochsch.; Avila, C.; Gomez, B.; Mendoza, L.; /Andes U., Bogota /Argonne /Arizona U. /Athens U. /Barcelona, IFAE /Baylor U. /Bonn U. /Boston U. /Brandeis U.

    2010-01-01

    We combine searches by the CDF and D0 collaborations for a Higgs boson decaying to W{sup +}W{sup -}. The data correspond to an integrated total luminosity of 4.8 (CDF) and 5.4 (D0) fb{sup -1} of p{bar p} collisions at {radical}s = 1.96 TeV at the Fermilab Tevatron collider. No excess is observed above background expectation, and resulting limits on Higgs boson production exclude a standard-model Higgs boson in the mass range 162-166 GeV at the 95% C.L.

  16. Top quarks at the Tevatron: Measurements of the top quark production and decay with the D0 experiment

    Energy Technology Data Exchange (ETDEWEB)

    Strandberg, Jonas [Stockholm Univ. (Sweden)

    2006-01-01

    This thesis presents two measurements of the to pquark using 230 pb-1 of data recorded with the D0 detector at the Tevatron accelerator. The first measurement determines the top pair production cross section at √s = 1.96 TeV in proton-antiproton collisions. In the standard model of particle physics the top quark decays almost exclusively into a W boson and a b quark. Candidate events are selected by requiring that at least one jet in the event is tagged with the secondary vertex algorithm.

  17. Combination of Tevatron searches for the standard model Higgs boson in the W+W- decay mode.

    Science.gov (United States)

    Aaltonen, T; Abazov, V M; Abbott, B; Abolins, M; Acharya, B S; Adams, M; Adams, T; Adelman, J; Aguilo, E; Alexeev, G D; Alkhazov, G; Alton, A; Alvarez González, B; Alverson, G; Alves, G A; Amerio, S; Amidei, D; Anastassov, A; Ancu, L S; Annovi, A; Antos, J; Aoki, M; Apollinari, G; Appel, J; Apresyan, A; Arisawa, T; Arnoud, Y; Arov, M; Artikov, A; Asaadi, J; Ashmanskas, W; Askew, A; Asman, B; Atramentov, O; Attal, A; Aurisano, A; Avila, C; Azfar, F; BackusMayes, J; Badaud, F; Badgett, W; Bagby, L; Baldin, B; Bandurin, D V; Banerjee, S; Barbaro-Galtieri, A; Barberis, E; Barfuss, A-F; Baringer, P; Barnes, V E; Barnett, B A; Barreto, J; Barria, P; Bartlett, J F; Bartos, P; Bassler, U; Bauer, D; Bauer, G; Beale, S; Bean, A; Beauchemin, P-H; Bedeschi, F; Beecher, D; Begalli, M; Begel, M; Behari, S; Belanger-Champagne, C; Bellantoni, L; Bellettini, G; Bellinger, J; Benitez, J A; Benjamin, D; Beretvas, A; Beri, S B; Bernardi, G; Bernhard, R; Bertram, I; Besançon, M; Beuselinck, R; Bezzubov, V A; Bhat, P C; Bhatnagar, V; Bhatti, A; Binkley, M; Bisello, D; Bizjak, I; Blair, R E; Blazey, G; Blessing, S; Blocker, C; Bloom, K; Blumenfeld, B; Bocci, A; Bodek, A; Boehnlein, A; Boisvert, V; Boline, D; Bolton, T A; Boos, E E; Borissov, G; Bortoletto, D; Bose, T; Boudreau, J; Boveia, A; Brandt, A; Brau, B; Bridgeman, A; Brigliadori, L; Brock, R; Bromberg, C; Brooijmans, G; Bross, A; Brown, D; Brubaker, E; Bu, X B; Buchholz, D; Budagov, J; Budd, H S; Budd, S; Buehler, M; Buescher, V; Bunichev, V; Burdin, S; Burkett, K; Burnett, T H; Busetto, G; Bussey, P; Buszello, C P; Buzatu, A; Byrum, K L; Cabrera, S; Calancha, C; Calfayan, P; Calpas, B; Calvet, S; Camacho-Pérez, E; Camarda, S; Cammin, J; Campanelli, M; Campbell, M; Canelli, F; Canepa, A; Carls, B; Carlsmith, D; Carosi, R; Carrasco-Lizarraga, M A; Carrera, E; Carrillo, S; Carron, S; Casal, B; Casarsa, M; Casey, B C K; Castilla-Valdez, H; Castro, A; Catastini, P; Cauz, D; Cavaliere, V; Cavalli-Sforza, M; Cerri, A; Cerrito, L; Chakrabarti, S; Chakraborty, D; Chan, K M; Chandra, A; Chang, S H; Chen, Y C; Chertok, M; Cheu, E; Chevalier-Théry, S; Chiarelli, G; Chlachidze, G; Chlebana, F; Cho, K; Cho, D K; Cho, S W; Choi, S; Chokheli, D; Chou, J P; Choudhary, B; Christoudias, T; Chung, K; Chung, W H; Chung, Y S; Chwalek, T; Cihangir, S; Ciobanu, C I; Ciocci, M A; Claes, D; Clark, A; Clark, D; Clutter, J; Compostella, G; Convery, M E; Conway, J; Cooke, M; Cooper, W E; Corbo, M; Corcoran, M; Cordelli, M; Couderc, F; Cousinou, M-C; Cox, C A; Cox, D J; Crescioli, F; Cuenca Almenar, C; Cuevas, J; Culbertson, R; Cully, J C; Cutts, D; Cwiok, M; Dagenhart, D; d'Ascenzo, N; Das, A; Datta, M; Davies, G; Davies, T; De, K; de Barbaro, P; De Cecco, S; Deisher, A; de Jong, S J; De la Cruz-Burelo, E; Déliot, F; Dell'Orso, M; De Lorenzo, G; Deluca, C; Demarteau, M; Demina, R; Demortier, L; Deng, J; Deninno, M; Denisov, D; Denisov, S P; d'Errico, M; Desai, S; DeVaughan, K; Di Canto, A; Diehl, H T; Diesburg, M; Di Ruzza, B; Dittmann, J R; Dominguez, A; Donati, S; Dong, P; D'Onofrio, M; Dorigo, T; Dorland, T; Dube, S; Dubey, A; Dudko, L V; Duflot, L; Duggan, D; Duperrin, A; Dutt, S; Dyshkant, A; Eads, M; Ebina, K; Edmunds, D; Elagin, A; Ellison, J; Elvira, V D; Enari, Y; Eno, S; Erbacher, R; Errede, D; Errede, S; Ershaidat, N; Eusebi, R; Evans, H; Evdokimov, A; Evdokimov, V N; Facini, G; Fang, H C; Farrington, S; Fedorko, W T; Feild, R G; Feindt, M; Ferapontov, A V; Ferbel, T; Fernandez, J P; Ferrazza, C; Fiedler, F; Field, R; Filthaut, F; Fisher, W; Fisk, H E; Flanagan, G; Forrest, R; Fortner, M; Fox, H; Frank, M J; Franklin, M; Freeman, J C; Fuess, S; Furic, I; Gadfort, T; Galea, C F; Gallinaro, M; Galyardt, J; Garberson, F; Garcia, J E; Garcia-Bellido, A; Garfinkel, A F; Garosi, P; Gavrilov, V; Gay, P; Geist, W; Geng, W; Gerbaudo, D; Gerber, C E; Gerberich, H; Gerdes, D; Gershtein, Y; Gessler, A; Giagu, S; Giakoumopoulou, V; Giannetti, P; Gibson, K; Gillberg, D; Gimmell, J L; Ginsburg, C M; Ginther, G; Giokaris, N; Giordani, M; Giromini, P; Giunta, M; Giurgiu, G; Glagolev, V; Glenzinski, D; Gold, M; Goldschmidt, N; Golossanov, A; Golovanov, G; Gómez, B; Gomez, G; Gomez-Ceballos, G; Goncharov, M; González, O; Gorelov, I; Goshaw, A T; Goulianos, K; Goussiou, A; Grannis, P D; Greder, S; Greenlee, H; Greenwood, Z D; Gregores, E M; Grenier, G; Gresele, A; Grinstein, S; Gris, Ph; Grivaz, J-F; Grohsjean, A; Grosso-Pilcher, C; Group, R C; Grundler, U; Grünendahl, S; Grünewald, M W; Guimaraes da Costa, J; Gunay-Unalan, Z; Guo, F; Guo, J; Gutierrez, G; Gutierrez, P; Haas, A; Haber, C; Haefner, P; Hagopian, S; Hahn, S R; Haley, J; Halkiadakis, E; Hall, I; Han, B-Y; Han, J Y; Han, L; Happacher, F; Hara, K; Harder, K; Hare, D; Hare, M; Harel, A; Harr, R F; Hartz, M; Hatakeyama, K; Hauptman, J M; Hays, C; Hays, J; Hebbeker, T; Heck, M; Hedin, D; Hegeman, J G; Heinrich, J; Heinson, A P; Heintz, U; Hensel, C; Heredia-De la Cruz, I; Herndon, M; Herner, K; Hesketh, G; Heuser, J; Hewamanage, S; Hidas, D; Hildreth, M D; Hill, C S; Hirosky, R; Hirschbuehl, D; Hoang, T; Hobbs, J D; Hocker, A; Hoeneisen, B; Hohlfeld, M; Hossain, S; Houben, P; Hou, S; Houlden, M; Hsu, S-C; Hu, Y; Hubacek, Z; Hughes, R E; Hurwitz, M; Husemann, U; Huske, N; Hussein, M; Huston, J; Hynek, V; Iashvili, I; Illingworth, R; Incandela, J; Introzzi, G; Iori, M; Ito, A S; Ivanov, A; Jabeen, S; Jaffré, M; Jain, S; James, E; Jamin, D; Jang, D; Jayatilaka, B; Jeon, E J; Jesik, R; Jha, M K; Jindariani, S; Johns, K; Johnson, C; Johnson, M; Johnson, W; Johnston, D; Jonckheere, A; Jones, M; Jonsson, P; Joo, K K; Jun, S Y; Jung, J E; Junk, T R; Juste, A; Kajfasz, E; Kamon, T; Karchin, P E; Kar, D; Karmanov, D; Kasper, P A; Kato, Y; Katsanos, I; Kaushik, V; Kehoe, R; Kephart, R; Kermiche, S; Ketchum, W; Keung, J; Khalatyan, N; Khanov, A; Kharchilava, A; Kharzheev, Y N; Khatidze, D; Khotilovich, V; Kilminster, B; Kim, D H; Kim, H S; Kim, H W; Kim, J E; Kim, M J; Kim, S B; Kim, S H; Kim, Y K; Kimura, N; Kirby, M H; Kirsch, L; Kirsch, M; Klimenko, S; Kohli, J M; Kondo, K; Kong, D J; Konigsberg, J; Korytov, A; Kotwal, A V; Kozelov, A V; Kraus, J; Kreps, M; Kroll, J; Krop, D; Krumnack, N; Kruse, M; Krutelyov, V; Kuhr, T; Kulkarni, N P; Kumar, A; Kupco, A; Kurata, M; Kurca, T; Kuzmin, V A; Kvita, J; Kwang, S; Laasanen, A T; Lam, D; Lami, S; Lammel, S; Lammers, S; Lancaster, M; Lander, R L; Landsberg, G; Lannon, K; Lath, A; Latino, G; Lazzizzera, I; Lebrun, P; LeCompte, T; Lee, E; Lee, H S; Lee, H S; Lee, J S; Lee, S W; Lee, W M; Leflat, A; Lellouch, J; Leone, S; Lewis, J D; Li, L; Li, Q Z; Lietti, S M; Lim, J K; Linacre, J; Lincoln, D; Lin, C-J; Lindgren, M; Linnemann, J; Lipaev, V V; Lipeles, E; Lipton, R; Lister, A; Litvintsev, D O; Liu, C; Liu, T; Liu, Y; Liu, Z; Lobodenko, A; Lockyer, N S; Loginov, A; Lokajicek, M; Lovas, L; Love, P; Lubatti, H J; Lucchesi, D; Lueck, J; Lujan, P; Lukens, P; Luna-Garcia, R; Lungu, G; Lyon, A L; Lysak, R; Lys, J; Maciel, A K A; Mackin, D; MacQueen, D; Madrak, R; Maeshima, K; Magaña-Villalba, R; Makhoul, K; Maksimovic, P; Mal, P K; Malde, S; Malik, S; Malik, S; Malyshev, V L; Manca, G; Manousakis-Katsikakis, A; Maravin, Y; Margaroli, F; Marino, C; Marino, C P; Martin, A; Martin, V; Martínez, M; Martínez-Ballarín, R; Martínez-Ortega, J; Mastrandrea, P; Mathis, M; Mättig, P; Mattson, M E; Mazzanti, P; McCarthy, R; McFarland, K S; McGivern, C L; McIntyre, P; McNulty, R; Mehta, A; Mehtala, P; Meijer, M M; Melnitchouk, A; Mendoza, L; Menezes, D; Menzione, A; Mercadante, P G; Merkin, M; Mesropian, C; Meyer, A; Meyer, J; Miao, T; Mietlicki, D; Miladinovic, N; Miller, R; Mills, C; Milnik, M; Mitra, A; Mitselmakher, G; Miyake, H; Moed, S; Moggi, N; Mondal, N K; Mondragon, M N; Moon, C S; Moore, R; Morello, M J; Morlock, J; Moulik, T; Movilla Fernandez, P; Muanza, G S; Mukherjee, A; Mulhearn, M; Muller, Th; Mülmenstädt, J; Mundal, O; Mundim, L; Murat, P; Mussini, M; Nachtman, J; Nagai, Y; Naganoma, J; Nagy, E; Naimuddin, M; Nakamura, K; Nakano, I; Napier, A; Narain, M; Nayyar, R; Neal, H A; Negret, J P; Nett, J; Neu, C; Neubauer, M S; Neubauer, S; Neustroev, P; Nielsen, J; Nilsen, H; Nodulman, L; Nogima, H; Norman, M; Norniella, O; Novaes, S F; Nunnemann, T; Nurse, E; Oakes, L; Obrant, G; Oh, S H; Oh, Y D; Oksuzian, I; Okusawa, T; Onoprienko, D; Orava, R; Orduna, J; Osman, N; Osta, J; Osterberg, K; Otec, R; Otero y Garzón, G J; Owen, M; Padilla, M; Padley, P; Pagan Griso, S; Pagliarone, C; Palencia, E; Pangilinan, M; Papadimitriou, V; Papaikonomou, A; Paramanov, A A; Parashar, N; Parihar, V; Park, S-J; Park, S K; Parks, B; Parsons, J; Partridge, R; Parua, N; Pashapour, S; Patrick, J; Patwa, A; Pauletta, G; Paulini, M; Paus, C; Peiffer, T; Pellett, D E; Penning, B; Penzo, A; Perfilov, M; Peters, K; Peters, Y; Pétroff, P; Phillips, T J; Piacentino, G; Pianori, E; Piegaia, R; Pinera, L; Piper, J; Pitts, K; Plager, C; Pleier, M-A; Podesta-Lerma, P L M; Podstavkov, V M; Pol, M-E; Polozov, P; Pondrom, L; Popov, A V; Potamianos, K; Poukhov, O; Prewitt, M; Price, D; Prokoshin, F; Pronko, A; Protopopescu, S; Ptohos, F; Pueschel, E; Punzi, G; Pursley, J; Qian, J; Quadt, A; Quinn, B; Rademacker, J; Rahaman, A; Ramakrishnan, V; Rangel, M S; Ranjan, K; Ranjan, N; Ratoff, P N; Razumov, I; Redondo, I; Renkel, P; Renton, P; Renz, M; Rescigno, M; Rich, P; Richter, S; Rijssenbeek, M; Rimondi, F; Ripp-Baudot, I; Ristori, L; Rizatdinova, F; Robinson, S; Robson, A; Rodrigo, T; Rodriguez, T; Rogers, E; Rolli, S; Rominsky, M; Roser, R; Rossi, M; Rossin, R; Roy, P; Royon, C; Rubinov, P; Ruchti, R; Ruiz, A; Russ, J; Rusu, V; Rutherford, B; Saarikko, H; Safonov, A; Safronov, G; Sajot, G; Sakumoto, W K; Sánchez-Hernández, A; Sanders, M P; Sanghi, B; Santi, L; Sartori, L; Sato, K; Savage, G; Saveliev, V; Savoy-Navarro, A; Sawyer, L; Scanlon, T; Schaile, D; Schamberger, R D; Scheglov, Y; Schellman, H; Schlabach, P; Schliephake, T; Schlobohm, S; Schmidt, A; Schmidt, E E; Schmidt, M A; Schmidt, M P; Schmitt, M; Schwanenberger, C; Schwarz, T; Schwienhorst, R; Scodellaro, L; Scribano, A; Scuri, F; Sedov, A; Seidel, S; Seiya, Y; Sekaric, J; Semenov, A; Severini, H; Sexton-Kennedy, L; Sforza, F; Sfyrla, A; Shabalina, E; Shalhout, S Z; Shary, V; Shchukin, A A; Shears, T; Shepard, P F; Shimojima, M; Shiraishi, S; Shivpuri, R K; Shochet, M; Shon, Y; Shreyber, I; Simak, V; Simonenko, A; Sinervo, P; Sirotenko, V; Sisakyan, A; Skubic, P; Slattery, P; Slaughter, A J; Slaunwhite, J; Sliwa, K; Smirnov, D; Smith, J R; Snider, F D; Snihur, R; Snow, G R; Snow, J; Snyder, S; Soha, A; Söldner-Rembold, S; Somalwar, S; Sonnenschein, L; Sopczak, A; Sorin, V; Sosebee, M; Soustruznik, K; Spurlock, B; Squillacioti, P; Stanitzki, M; Stark, J; St Denis, R; Stelzer, B; Stelzer-Chilton, O; Stentz, D; Stolin, V; Stoyanova, D A; Strandberg, J; Strang, M A; Strauss, E; Strauss, M; Ströhmer, R; Strologas, J; Strom, D; Strycker, G L; Stutte, L; Suh, J S; Sukhanov, A; Suslov, I; Svoisky, P; Taffard, A; Takahashi, M; Takashima, R; Takeuchi, Y; Tanaka, R; Tanasijczuk, A; Tang, J; Taylor, W; Tecchio, M; Teng, P K; Thom, J; Thome, J; Thompson, G A; Thomson, E; Tiller, B; Tipton, P; Titov, M; Tkaczyk, S; Toback, D; Tokar, S; Tokmenin, V V; Tollefson, K; Tomura, T; Tonelli, D; Torre, S; Torretta, D; Totaro, P; Trovato, M; Tsai, S-Y; Tsybychev, D; Ttito-Guzmán, P; Tuchming, B; Tu, Y; Tully, C; Turini, N; Tuts, P M; Ukegawa, F; Unalan, R; Uozumi, S; Uvarov, L; Uvarov, S; Uzunyan, S; van den Berg, P J; Van Kooten, R; van Leeuwen, W M; van Remortel, N; Varelas, N; Varganov, A; Varnes, E W; Vasilyev, I A; Vataga, E; Vázquez, F; Velev, G; Vellidis, C; Verdier, P; Vertogradov, L S; Verzocchi, M; Vesterinen, M; Vidal, M; Vila, I; Vilanova, D; Vilar, R; Vint, P; Vogel, M; Vokac, P; Volobouev, I; Volpi, G; Wagner, P; Wagner, R G; Wagner, R L; Wagner, W; Wagner-Kuhr, J; Wahl, H D; Wakisaka, T; Wallny, R; Wang, M H L S; Wang, S M; Warburton, A; Warchol, J; Waters, D; Watts, G; Wayne, M; Weber, G; Weber, M; Weinberger, M; Weinelt, J; Wester, W C; Wetstein, M; White, A; Whitehouse, B; Whiteson, D; Wicke, D; Wicklund, A B; Wicklund, E; Wilbur, S; Williams, G; Williams, H H; Williams, M R J; Wilson, G W; Wilson, P; Wimpenny, S J; Winer, B L; Wittich, P; Wobisch, M; Wolbers, S; Wolfe, C; Wolfe, H; Wood, D R; Wright, T; Wu, X; Würthwein, F; Wyatt, T R; Xie, Y; Xu, C; Yacoob, S; Yagil, A; Yamada, R; Yamamoto, K; Yamaoka, J; Yang, U K; Yang, W-C; Yang, Y C; Yao, W M; Yasuda, T; Yatsunenko, Y A; Ye, Z; Yeh, G P; Yi, K; Yin, H; Yip, K; Yoh, J; Yoo, H D; Yorita, K; Yoshida, T; Youn, S W; Yu, G B; Yu, I; Yu, J; Yu, S S; Yun, J C; Zanetti, A; Zeitnitz, C; Zelitch, S; Zeng, Y; Zhang, X; Zhao, T; Zheng, Y; Zhou, B; Zhu, J; Zielinski, M; Zieminska, D; Zivkovic, L; Zucchelli, S; Zutshi, V; Zverev, E G

    2010-02-12

    We combine searches by the CDF and D0 Collaborations for a Higgs boson decaying to W+W-. The data correspond to an integrated total luminosity of 4.8 (CDF) and 5.4 (D0) fb(-1) of pp collisions at square root(s) = 1.96 TeV at the Fermilab Tevatron collider. No excess is observed above background expectation, and resulting limits on Higgs boson production exclude a standard model Higgs boson in the mass range 162-166 GeV at the 95% C.L.

  18. Analyse énonciative du point du vue, narration et analyse de discours

    Directory of Open Access Journals (Sweden)

    Alain Rabatel

    2007-01-01

    Full Text Available Cet article montre que l’analyse énonciative du point de vue (PDV, en rupture avec la typologie des focalisations de Genette, peut renouveler partiellement la narratologie, à la condition de substituter à l’approche immanentiste du récit une analyse interactionnelle de la narration. L’article présente d’abord l’approche énonciative du PDV, en appui des théories de Ducrot, et, sur cette base, propose diverses modalités de PDV (représenté, raconté, asserté qui donnent corps au point de vue des personnages ou du narrateur en modifiant sensiblement les analyses de Genette. Dans une deuxième partie, l’article envisage le rôle des PDV dans la narration, notamment dans la réévaluation des dimensions cognitive et pragmatique de la mimésis, puis dans les mécanismes inférentiels-interprétatifs, proches du système de sympathie de Jouve, enfin, dans la revalorisation du rôle du narrateur •puisque ce dernier se construit dans le même temps qu’il construit ses personnages.

  19. Prescrire du cannabis fumé pour la douleur chronique non cancéreuse

    Science.gov (United States)

    Kahan, Meldon; Srivastava, Anita; Spithoff, Sheryl; Bromley, Lisa

    2014-01-01

    qui prennent de fortes doses d’opioïdes ou de benzodiazépines (données probantes de niveau III). Il faut conseiller aux utilisateurs de cannabis d’attendre au moins 3 à 4 heures avant de conduire s’ils en ont fumé, au moins 6 heures s’ils en ont consommé par la bouche et au moins 8 heures s’ils ont ressenti un «high» subjectif (données probantes de niveau II). La dose maximale recommandée est de 1 inhalation 4 fois par jour (environ 400 mg par jour) de cannabis séché contenant 9 % de delta-9-tétrahydrocannabinol (données probantes de niveau III)). Les médecins devraient éviter de demander une consultation pour les patients auprès de cliniques «cannabinoïdes» (données probantes de niveau III). Conclusion Les lignes directrices futures devraient se fonder sur une révision systématique des ouvrages scientifiques sur la sécurité et l’efficacité du cannabis fumé. D’autres recherches sont nécessaires sur l’efficacité et la sécurité à long terme du cannabis fumé par rapport à d’autres cannabinoïdes pharmaceutiques, aux opioïdes et à d’autres analgésiques standards.

  20. Les métamorphoses du pouvoir

    OpenAIRE

    Adler, Alfred

    2004-01-01

    On sait que la sorcellerie en Afrique peut s'exercer du faible au fort ou l'inverse. Les situations qui sont ici analysées sont celles où les rois ou les chefs sont expressément désignés comme sorciers, soit qu'ils le deviennent du fait même de leur investiture, soit qu'il leur ait fallu le devenir pour accéder au pouvoir et le conserver face à des rivaux usant des mêmes moyens. Quoi qu'il en soit, un roi-sorcier offre une figure paradoxale du pouvoir, et cela doublement : garant de l'...

  1. Oncoplastie avec conservation mammaire dans le traitement du cancer du sein: à propos de 16 cas

    OpenAIRE

    2015-01-01

    Le cancer du sein est actuellement le cancer le plus fréquent chez la femme, et pose un véritable problème diagnostique et thérapeutique. Le dépistage des lésions à un stade de plus en plus précoce, a permis une extension des indications du traitement conservateur radiochirurgical, qui était initialement limitées aux tumeurs de moins de 3 cm, unifocales, non inflammatoires. Par ailleurs, l'utilisation de traitements préopératoires permet d’étendre les indications du traitement conservateur à ...

  2. Search for supersymmetric particles in the dimuon channels with the D-Zero experiment at the Tevatron; Recherche de particules supersymetriques dans les canaux dimuons avec le detecteur D-Zero au TeVatron

    Energy Technology Data Exchange (ETDEWEB)

    Vu Anh, T

    2004-07-01

    Supersymmetry is a possible way for physics beyond the standard model. This work is dedicated to the search of supersymmetric particles such as squarks and gluinos at the Tevatron collider. The analysis has been made on experimental data from the run-II. The first chapter is dedicated to a brief presentation of the standard model. In the second chapter the author reviews the recent work on this issue in CERN (Lep) and in Fermilab (Tevatron). The experimental properties of the search for squarks and gluinos such as the signature with leptons in the final state are detailed in this chapter. The third chapter is devoted to the D0 detector and to the reconstruction of particles with it. The fourth chapter describes the specificity of this work : the detection of squarks and gluinos through the simplest signature possible: 2 muons, 2 jets and with the adequate missing energy in the final state. It appears that for an integrated luminosity of 170 pb{sup -1} no events in excess with respect to the standard model has been detected. As a consequence it is shown that squarks and gluinos must have a mass greater than 200-250 GeV. (A.C.)

  3. Forward-Backward Asymmetry of Top Quark Pair Productionn at the Fermilab Tevatron

    Energy Technology Data Exchange (ETDEWEB)

    Hong, Ziqing [Texas A & M Univ., College Station, TX (United States)

    2015-12-01

    This dissertation presents the final measurements of the forward-backward asymmetry (AFB) of top quark-antiquark pair events (t t-) at the Collider Detector at Fermilab (CDF) experiment. The t t- events are produced in proton{anti-proton collisions with a center of mass energy of 1:96 TeV during the Run II of the Fermilab Tevatron. The measurements are performed with the full CDF Run II data (9.1 fb-1) in the final state that contain two charged leptons (electrons or muons, the dilepton final state), and are designed to con rm or deny the evidence-level excess in the AFB measurements in the final state with a single lepton and hadronic jets (lepton+jets final state) as well as the excess in the preliminary measurements in the dilepton final state with the first half of the CDF Run II data. New measurements include the leptonic AFB (AlFB), the lepton-pair AFB (All FB) and the reconstructed top AFB (At t FB). Each are combined with the previous results from the lepton+jets final state measured at the CDF experiment. The inclusive Al FB, All FB, and At t FB measured in the dilepton final state are 0.072 ± 0.060, 0.076 ± 0.081, and 0.12 ± 0.13, to be compared with the Standard Model (SM) predictions of 0.038 ± 0.003, 0.048 ± 0.004, and 0.010 ± 0.006, respectively. The CDF combination of AlFB and At t FB are 0.090+0:028 -0.026, and 0.160 ± 0.045, respectively. The overall results are consistent with the SM predictions.

  4. Le Flaubert de Charles Du Bos

    Directory of Open Access Journals (Sweden)

    Jacques Neefs

    2009-01-01

    Full Text Available Charles Du Bos a porté une attention constante à l’œuvre de Flaubert (à l’exclusion de Bouvard et Pécuchet qui semble ne pas exister pour lui, à Madame Bovary et à L’Éducation sentimentale en particulier. La mise en relation de son étude : « Sur le milieu intérieur chez Flaubert », écrite en 1921, avec des textes du Journal de 1923 et de 1937, les rapprochements avec Gogol, Thomas Hardy, Tolstoï, Baudelaire, Henry James qui traversent les écrits de Du Bos, permettent de suivre ce que celui-ci décrit comme « l’expérience spirituelle » d’une matérialité comprise dans la conquête de la triple exigence du Beau, du Vivant et du Vrai. Du Bos décèle la force de l’œuvre de Flaubert dans la « disproportion » du style, et dans la puissance d’absorption qui fait la densité de cette prose, et qui désigne un extraordinaire travail de conversion. L’obscure expérience spirituelle ainsi poursuivie est celle d’un absolu de l’art, expérience paradoxale d’un « mystique qui ne croit à rien » (comme se désignait Flaubert lui-même, que le critique lie à une interrogation sur sa propre conversion.Charles Du Bos devoted an unflagging attention to Flaubert’s work (except for Bouvard et Pécuchet, which, apparently, according to him did not exist, to Madame Bovary and in particular L’Éducation sentimentale. The connection between his essay “Sur le milieu intérieur chez Flaubert”, written in 1921, and extracts from his Journal, from 1923 to 1937, the comparisons with Gogol, Thomas Hardy, Tolstoy, Baudelaire, and Henry James that run through the writings of Du Bos, allow us to follow what he terms “the spiritual experience” of a materiality encompassed in the conquest of the triple demand of the Beautiful, the Living, the Truth. Du Bos detects the power of Flaubert’s work in the “disproportion” of his style, and the power of absorption that forms the density of his prose, showing an

  5. Measurements of beam halo diffusion and population density in the Tevatron and in the Large Hadron Collider

    Energy Technology Data Exchange (ETDEWEB)

    Stancari, Giulio [Fermilab

    2015-03-01

    Halo dynamics influences global accelerator performance: beam lifetimes, emittance growth, dynamic aperture, and collimation efficiency. Halo monitoring and control are also critical for the operation of high-power machines. For instance, in the high-luminosity upgrade of the LHC, the energy stored in the beam tails may reach several megajoules. Fast losses can result in superconducting magnet quenches, magnet damage, or even collimator deformation. The need arises to measure the beam halo and to remove it at controllable rates. In the Tevatron and in the LHC, halo population densities and diffusivities were measured with collimator scans by observing the time evolution of losses following small inward or outward collimator steps, under different experimental conditions: with single beams and in collision, and, in the case of the Tevatron, with a hollow electron lens acting on a subset of bunches. After the LHC resumes operations, it is planned to compare measured diffusivities with the known strength of transverse damper excitations. New proposals for nondestructive halo population density measurements are also briefly discussed.

  6. L’ombre du Condor

    Directory of Open Access Journals (Sweden)

    Franck Gaudichaud

    2003-09-01

    Full Text Available Si l’on observe aujourd’hui, avec un regard d’historien, le Cône Sud à la fin des années soixante soixante-dix et que par, la suite, on tourne une page de quelques années, pour fixer la même partie du monde, le constat est sans appel : le sous-continent latino-américain est passé, en général, d’une phase de forte mobilisation et politisation sociale, montée en puissance de partis et organisations révolutionnaires, surgissements de gouvernements populistes de gauche ou progressistes – appelant à une rupture avec l’impérialisme –, à un reflux généralisé du mouvement ouvrier, une ère de violence politique étatisée, la destruction massive de tous les espaces d’expression et de participation démocratiques, l’écrasement physique et idéologique sans relâche des militants et mouvements révolutionnaires, la mise en place de modèles économiques capitalistes dirigistes puis/ou néolibéraux. Que s’est-il passé ? Quel fil conducteur a été rompu et par quels moyens l’Amérique Latine a été conduite à ce reflux des luttes sociales ? Pour répondre à cette question, nous nous contenterons dans cet article de focaliser notre objectif sur un aspect spécifique et essentiel de ce retournement de tendance que vit alors l���Amérique Latine : celui de la mise en place d’un terrorisme d’Etat contre-révolutionnaire transnational, appuyé par l’impérialisme américain, nommé « l’Opération Condor ». Dans cet article, il s’agit de montrer le fonctionnement d’un terrorisme hégémonique dont l’impact sur les sociétés latino-américaines est considérable en termes de destruction du mouvement social, des activités culturelles et de l’ensemble de la vie sociale et politique qui restent marquées, encore aujourd’hui à des degrés divers, par la violence, la peur et l’atomisation structurelle.Si miramos hoy en día, desde una perspectiva histórica, el Cono Sur hacia finales de

  7. CONTROLE DU RISQUE ET EXPERTISE : France : la précaution entre expertise et débat public Le cas des plantes transgéniques

    Directory of Open Access Journals (Sweden)

    Roy Alexis

    2000-07-01

    Full Text Available Depuis 1996, la commercialisation des premières plantes transgéniques s’est accompagnée d’un large débat en France (et en Europe. La controverse qui s’est ainsi développée a été le théâtre d’un processus d’appropriation par des acteurs hétérogènes de questions qui avaient été jusqu’alors essentiellement traitées par un cercle restreint d’intervenants réunis autour de quelques instances officielles de contrôle, dont principalement la Commission du génie biomoléculaire (CGB chargée de délivrer des avis auprès des instances exécutives concernant la dissémination dans l’environnement des organismes génétiquement modifiés (OGM. Une partie des critiques émises a porté sur les évaluations qui ont conduit à autoriser ces mises sur le marché ainsi que sur le fonctionnement de la CGB. Le gouvernement français a tenté de traduire cette demande d’ouverture du processus de décision à travers l’invocation du principe de précaution. L’extension de l’espace des débats a ainsi contribué à replacer la question des risques liés aux plantes transgéniques dans une réflexion élargie aux modèles de développement agricole et à l’alimentation. La rupture ainsi amorcée avec un modèle linéaire de la décision offre l’opportunité d’explorer le rôle qu’y remplissent les experts et les évolutions que pourrait impulser l’application du principe de précaution. En effet, de plus en plus présentée comme un nouveau paradigme en termes de politique environnementale et sanitaire, la précaution impliquerait une modification des liens unissant l’expertise scientifique et la décision. Fondant l’intervention publique sur la prise en compte des indéterminations, on peut toutefois se demander dans quelle mesure l’instrumentalisation de ce principe est limitée par une culture scientifique du risque encore dominée par une appropriation linéaire et déterministe de l’incertitude ? Si la

  8. Utilisation du langage signal pour l'etude d'algorithmes de traitement du Signal electrocardiographique

    OpenAIRE

    Médigue, Claire; Clairambault, Jean; Kauffmann, François; Sorine, Michel; Cursi-Dascalova, Lilia

    1992-01-01

    Projet SOSSO; Pour etudier la maturation du Systeme Nerveux Autonome (SNA) chez les nouveaux nes, on analyse la Variabilite du Rythme Cardiaque (VRC), en relation avec d'autres informations biologiques telles que les changements de stades de sommeil. La VRC est calculee par la Transformee de Fourier a Court Terme dans trois bandes de frequence : la haute frequence, refletant le controle para sympathique seul et liee au cycle respiratoire ; les moyenne et basse frequences, refletant a la fois ...

  9. OGM : vers une définition commune du contenu du problème ?

    Directory of Open Access Journals (Sweden)

    Icart Jean-Claude

    2001-07-01

    Full Text Available Les divergences croissantes depuis des années entre experts, responsables économiques, et acteurs sociaux et « citoyens » au sujet des OGM, ont pu être analysées à juste titre, comme exprimant la difficulté de dégager une « définition commune du contenu du problème »1.

  10. Clinical Application of the Du Channel

    Institute of Scientific and Technical Information of China (English)

    刘淑娅; 王世杰

    2003-01-01

    @@ The authors have, in recent years, obtained quite good therapeutic results in their acupuncture treatment of mental diseases, heat syndromes and cerebrovascular diseases through treating mainly the Du Channel with the methods of resuscitating and regulating the mind, and clearing and activating the channels and collaterals. The illustrative cases are reported below.

  11. ESTIMATION DU MODELE LINEAIRE GENERALISE ET APPLICATION

    Directory of Open Access Journals (Sweden)

    Malika CHIKHI

    2012-06-01

    Full Text Available Cet article présente  le modèle linéaire généralisé englobant les  techniques de modélisation telles que la régression linéaire, la régression logistique, la régression  log linéaire et la régression  de Poisson . On Commence par la présentation des modèles  des lois exponentielles pour ensuite estimer les paramètres du modèle par la méthode du maximum de vraisemblance. Par la suite on teste les coefficients du modèle pour voir leurs significations et leurs intervalles de confiances, en utilisant le test de Wald qui porte sur la signification  de la vraie valeur du paramètre  basé sur l'estimation de l'échantillon.

  12. Développement durable et agriculture durable : sens du concept de « durabilité » à travers la presse régionale et le discours des agriculteurs

    Directory of Open Access Journals (Sweden)

    Lise Bihannic

    2011-12-01

    Full Text Available Cette étude porte sur la question du sens des concepts de développement durable et d’agriculture durable à travers, d’une part, une analyse de contenu de leur diffusion dans la presse régionale (presse spécialisée en milieu agricole et presse généraliste. D’autre part, elle s’intéresse à l’appropriation de ces concepts par les agriculteurs. Pour ce faire, des entretiens semi-directifs ont été menés auprès de ces acteurs en prise avec ces questions de « durabilité ». L’objectif est de mettre en parallèle ces deux formes de contenu et de mettre en lumière les représentations sociales liées à ces objets en partant du postulat que ces dernières, en tant que forme de connaissance socialement élaborées, sont un guide pour l’action et que celles-ci se forment, se transmettent, et évoluent au cœur de la communication (Moscovici, 1976.This study focuses on the meaning of the concepts of sustainable development and sustainable agriculture. First, this study deals with a content analysis of their circulation in the regional papers (specialized in agriculture and popular newspaper. Second, it is interested in the appropriation of theses concepts farmers. Semi-structured interviews were carried out with these stakeholders concerned with these issues. The aim of the study is to compare these two content analyses and to highlight the social representations of these concepts. We postulate that these representations are a form of knowledge which is socially constructed. They are a guide to action and that they take shape, they are transmitted and they evolve in the heart of communication (Moscovici, 1976.

  13. Néotoponymie contestée à Potchefstroom / Tlokwe (Province du Nord-Ouest, Afrique du Sud

    Directory of Open Access Journals (Sweden)

    Myriam Houssay-Holzschuch

    2010-09-01

    Full Text Available Illustration 1 - Extrait du site de la municipalité de Potchefstroom / TlokweSource : http://www.potch.co.za/newsarchive/streetnames.htmlIllustration 2- Potchefstroom (Afrique du SudAuteur : Béatrice Obry-Guyot, début décembre 2007.Illustration 3 - Extrait du plan Google Map de PotchefstroomSource : Google Map.La question toponymique en Afrique du Sud sur la longue durée porte sur deux thèmes essentiels porteurs de controverses : le plurilinguisme et le marquage symbolique et mémoriel du te...

  14. Sébastien Broca, Utopie du logiciel libre. Du bricolage informatique à la réinvention sociale

    OpenAIRE

    Goëta, Samuel

    2014-01-01

    Traitant des pratiques et des conceptions du logiciel libre mais aussi, plus largement, du mouvement pour l’ouverture des savoirs, Utopie du logiciel libre ambitionne, premièrement, de nourrir une réflexion critique sur l’ethos du libre au sens d’un « ensemble de valeurs qui constituent un cadre pour l’action et s’actualisent dans des pratiques » (p. 24) et, deuxièmement, d’élaborer une sociologie critique du libre. Reprenant la notion d’utopie concrète chez Ernst Bloch (Le principe Espérance...

  15. Esquisse du parlementarisme et du monopartisme en Afrique: le cas du Togo

    Directory of Open Access Journals (Sweden)

    E. A. B. van Rouveroy van Nieuwaal

    1989-01-01

    Full Text Available Witnessed the last hundred years profound political and constitutional changes. In this respect there are many differences between African States depending on which kind of colonial overlord has been the ruling power. The African State was a juridical entity in international law, but was it also, at the time of independence, an empirical entity in national fact?In almost all cases the empirical reality as a functioning government was still primarily the presence of European bureaucrats who has embodied the colonial state. Independence therefore opened a gap between the international legitimacy and the internal marginality of many emergent African State. The gap often presented a real political dilemma to the new African rulers: they usually could retain European officials only by compromising their national independence and could dispense with them only at the risk of undermining governmental performance. After adoption of European constitutional law and with, initially, a high degree of similarity between most constitutions in French-speaking Africa, nowadays these constitutions differ widely, contrary to the Commonwealth Africa that has experienced fewer innovations and constitutional breakdowns.Parliamentary systems of government gave way to One Party Systems, introduced in many cases by the national army, as the best equiped, trained, paid and organised power in the country. This has been the political and constitutional development in Togo as well. Since 1969, it has a One Party System, the Rassemblement du Peuple Togolais, founded by the President of the Togolese Republic, Gen. Gnassingbé Eyadéma. But, as everywhere else, doubts are growing about the effectiveness of the One Party System. Are the Togolese perspectives such that Eyadéma is willing to have an open mind and to be all ears for the critics to his own creation? Another intriguing question is to know in which way the Africantraditional authorities (" chieftancy", as the core

  16. Choix du sujet de mémoire par l’étudiant et effets sur la relation pédagogique de direction de mémoire en Master : apprendre à faire le « deuil » du projet de recherche « idéal »

    Directory of Open Access Journals (Sweden)

    Laetitia Gérard

    2011-01-01

    Full Text Available Cet article porte sur l’une des caractéristiques du diplôme de Master Recherche en Sciences de l'éducation qui diffère de la Licence : l’accentuation de la part d’autodirection de l’étudiant dans sa formation, qui débute par la prise en charge du choix de son sujet de mémoire. On s’interroge sur la manière dont l’étudiant s’approprie ce nouveau rôle qui lui est « offert » à l’entrée en Master. Des entretiens semi-directifs ont été menés auprès de vingt binômes « directeur de mémoire-étudiant » appartenant à la discipline des Sciences de l'éducation, dans cinq universités différentes. Les résultats montrent qu’il y a un gap entre le projet de recherche initialement envisagé par l’étudiant « masterant » et le projet de recherche tel qu’il est attendu à ce niveau universitaire. Ce gap est à l’origine de tensions au sein du binôme si l’étudiant n’accepte pas de « faire le deuil » de son projet de recherche « idéal ».This article addresses one of the characteristics of the French Master’s degree in educational sciences, which makes it different from the Bachelor’s degree. Self-directed learning progressively increases in the way the student works, starting with his/her own choice of a research topic. I studied the way the student fits this new role. Semi-directed interviews were carried out with eighteen “supervisor-student” pairs in the discipline of educational sciences, in five different universities. The results show that there is a difference between the initial research that the student would like to lead and the research which is expected at Master’s degree. This gap leads to tension within the pedagogical relationship if the student does not accept to let go of his original ”ideal” research.

  17. Rare decays of B mesons and baryons at the Tevatron and the LHC

    Energy Technology Data Exchange (ETDEWEB)

    Volpi, Guido [Univ. of Siena (Italy)

    2008-07-01

    The experimental study of rare decays of hadrons containing the b quark has been a fertile ground for some time, and keeps being one of the most interesting subjects in high energy physics. It has improved our understanding of hadronic processes, and allows investigating various aspects of the Standard Model and searching for hints of physics beyond the Standard Model. Examples are the comparison of branching fractions of charmless modes with predictions of models, the constraints on CKM angles (B0 → π+π-, B → DK, with D in suppressed modes), the observation of purely leptonic modes (B± → τ±v), the recently established difference in ACP between B0 → K+π- and B± → K±π0, suspected to be a hint new physics. All of them came from a long and successful experimental activity with e+e- collisions at the Y(4S) resonance. With hadronic colliders now coming into play, the study of rare decays is reaching new heights. Given the high cross section for production of all kinds of B hadrons, the record luminosities now provided by the Tevatron collider, and the LHC program in view for the next years, there is the potential for a rich program of interesting new measurements, including even rarer modes as the Bs0 → μ+μ-, strongly suppressed in the standard model but very sensitive to many NP scenarios. The complexity of the hadronic collision environment, however, requires detectors with high precision and high quality tracking, and a trigger system capable of complex event selections at high rates. The CDF experiment, thanks to a fast trigger on impact parameter, has been able to reconstruct many rare B decays, including previously unobserved modes Bs0 → K+K- and Bs0 → K

  18. Liens à l’origine et qualité spécifique d’un produit de l’artisanat agroalimentaire du Bénin – le kluiklui d’Agonlin

    Directory of Open Access Journals (Sweden)

    Videgla Euloge Grégoire

    2016-01-01

    Full Text Available Les kluiklui ou kwlikwli sont des bâtonnets frits de pâte d’arachide partiellement déshuilée qui entrent dans la consommation alimentaire régulière des Béninois. Leur production dépend de savoir-faire artisanaux régionalisés. Les plus typiques sont ceux de la région Agonlin. Mieux connaître les préférences des consommateurs africains est une des conditions de la promotion des filières de produits locaux. La fréquence de consommation ainsi que la capacité à différencier les origines et autres attributs de qualité ont été évaluées au moment de l’achat de kwlikwli d’Agonlin auprès de 150 consommateurs issus d’une part des zones urbaines et d’autre part du territoire Agonlin. Quarante pour cent de ces derniers consomment des kwlikwli plusieurs fois par semaine et plus encore pour les populations ayant les plus faibles revenus. Néanmoins, même les acheteurs démunis ont des exigences de qualité. Les acheteurs de kwlikwli d’Agonlin le choisissent délibérément face à une offre plus variée pour son bon goût, et en particulier son assaisonnement, son odeur et sa croustillance et s’assurent de sa qualité en choisissant une source d’approvisionnement leur garantissant un produit d’origine. Les consommateurs urbains sont fréquemment originaires de la région de production et entretiennent une relation fidélisée avec une revendeuse qui est elle-même en relation avec ce territoire. La consommation de kwlikwli renforce ainsi les liens des consommateurs avec leur zone d’origine. Cela constitue actuellement un atout auprès des migrants de première génération. Mais pour le futur, une stratégie plus active de construction d’un lien à l’origine pourrait être nécessaire.

  19. Les rues fermées : du collectif à la collectivité. Regards croisés Nantes/Recife Gated streets: from social affinity to community. Crossed looks Nantes/Recife

    Directory of Open Access Journals (Sweden)

    Fanny Vuaillat

    2012-06-01

    Full Text Available Cet article propose une analyse des rues fermées, publiques ou privées, dans deux contextes différents, Nantes en France et Recife au Brésil. Ce double regard analytique permet de s’extraire des effets de contextes pour tenter de percevoir le sens commun de ces rues dans la fabrique de la ville fermée. À partir d’une série d’observations et d’entretiens auprès de responsables techniques ou politiques des pouvoirs publics locaux, ainsi qu’auprès d’habitants, plusieurs rues fermées servent à appréhender la manière dont l’installation d’un obstacle au passage instaure une frontière qui impose un rapport négocié, non exempt de frictions, du collectif à constituer à la collectivité. Cette limite ne sert pas tant un entre-soi affinitaire, qu’elle ne préserve des intérêts communs, pour lesquels il s’agit de former un collectif. Il faut donc trouver un équilibre, qui s’avère être soit frictionnel, soit établi sur la base d’un consensus a minima. Mais les pouvoirs publics, avec un discours ambigu, laissent des marges de manœuvre à une négociation en initiant une gouvernance urbaine sur les bases de frontières, physiques et juridiques, malléables et poreuses.The article analyses restricted and gated streets in both different context, Nantes in France and Recife in Brazil. This double analysis minimizes the effects of context and tries to perceive generic meaning in the restricted city. Starting from observations and interviews with the representatives of local authorities and the dwellers, several examples are used to understand the installation of an obstacle which creates a border and imposes negotiation (not necessarily free from tensions between the dwellers group to be formed and the local authorities. This limit preserves a community of interest, more than a social affinity community. This kind of stability can be frictional or based on a soft consensus. Nevertheless, the ambiguous view of the

  20. Study of semi-leptonic decay of B meson, in the ways lvD{sup *} and lvD with ALEPH detector at LEP: measurement of the fragmentation function of b quark and search for D{sup **} states; Etude des desintegrations semi-leptoniques du meson B, dans les canaux D*lv et Dlv, aupres du detecteur ALEPH au LEP: mesure de la fonction de fragmentation du quark b et recherche d`etats D**

    Energy Technology Data Exchange (ETDEWEB)

    Bonis, I. de

    1994-06-01

    This work is dedicated to the measurement of the fragmentation function of the quark b, with the ALEPH detector, at LEP. The main aspects of this measure is to be as independent as possible from any model. For this, we reconstruct the semi-leptonic decay modes of the B meson, in the ways lvD deg., lvD{sup *+} and lvD{sup +}. In a first step, we describe the criteria used to select those modes. Then, we determine the fragmentation function by measuring the ratio X{sub B} = 2 E{sub B} / {radical} S, where E{sub B} is the B meson energy and {radical} s/2 the useful energy in the center of mass. The measure of E{sub B} needs a precise reconstruction of the neutrino energy, which is not detected. We present here the method that we used for this reconstruction. Once the acceptance correction is applied, we obtain, for the variable X{sub B}, a distribution with mean value: < X{sub B} > = 0.711 {+-} 0.009 (stat). To be as independent as possible of the model (Peterson function) used n the Monte-Carlo determination of the acceptance, we do an iterative calculation of the acceptance. We obtain < X{sub B}> = 0.712 {+-} 0.009(stat) {+-} 0.017 (syst). Furthermore, this measure depends of the D** contribution, badly known for now. Therefore, we search this contribution, using the events selected before, on the one hand by a direct observation, on the other hand by reconstructing the mass of the B meson. (author). 64 refs.

  1. La communication marketing intégrée auprès des entreprises de services : une étude de cas exploratoire dans l’hôtellerie

    OpenAIRE

    Menvielle, William

    2011-01-01

    Depuis le 11 septembre 2001, de nombreuses entreprises touristiques n’ont eu d’autres choix que de réduire leurs prix et de pousser les consommateurs à découvrir leur site Web. Face à cette démocratisation de la recherche d’information sur Internet et de l’utilisation des sites Web du secteur hôtelier et touristique à des fins d’information et d’achat, les consommateurs considèrent Internet non plus « comme une panacée […] mais comme un outil fonctionnel pouvant les aider ».Toutefois, les ent...

  2. L’autodétermination dans la mise en place de projet: regards croisés des animateurs socioculturels et des éducateurs sociaux sur leur partique auprès des personnes souffrant de troubles psychiques

    OpenAIRE

    2015-01-01

    Cette recherche exploratoire porte sur le thème de l’autodétermination dans la mise en place de projet avec des personnes qui souffrent de troubles psychiques. Nous avons axé notre démarche sous l’angle du travailleur social et plus particulièrement des animateurs socioculturels et des éducateurs sociaux. Le but de notre recherche est de mettre en lumière la manière dont les professionnels cités ci-dessus estiment favoriser l’autodétermination des personnes souffrant de troubles psychiques da...

  3. Du crépuscule à l’aube From dusk to dawn: Finding compromises in nurses’ night shifts

    Directory of Open Access Journals (Sweden)

    Cathy Toupin

    2009-07-01

    Full Text Available Parmi les caractéristiques du travail susceptibles d’influencer les processus de régulation en lien avec l’âge et l’expérience, les questions d’horaires sont peu abordées. Nous pensons cependant qu’une composante importante, dans la construction et la mobilisation de l’expérience, s’élabore en relation avec le type d’horaire. L’objectif de cette recherche est de caractériser, au travers d’une étude menée auprès d’infirmières d’un service de pneumologie français, les stratégies mises en œuvre par les personnels de nuit ; et de proposer une approche dynamique de l’articulation entre horaires et activité de travail, en repérant comment cette articulation s’est forgée au cours du parcours professionnel avec l’expérience, comment ce processus est « lisible » dans l’activité d’aujourd’hui. Les infirmières se « prescrivent » des buts d’actions, élaborent une acception nocturne de leur tâche compte tenu de l’état des patients (par exemple, but visant à respecter le sommeil des patients, à apaiser leurs angoisses, de l’environnement désert des services (par exemple, but visant à consolider sa connaissance de l’état des patients, et de leur état psychophysiologique (par exemple, but visant à maintenir la vigilance. L’expérience du travail de nuit va leur permettre, d’une part de reconnaître ces buts, et d’identifier les contradictions pouvant en émerger ; d’autre part de compenser les difficultés et perturbations provoquées par ces tensions, via l’élaboration de compromis.Among the work characteristics that are likely to influence age and experience related adjustment processes, the issue of work schedules remains largely unexplored. We believe however that work schedules or shifts play an important part in building and mobilizing experience. This paper aims at characterizing the specific strategies implemented by night shift personnel based on a study

  4. J/ψ polarization at the Tevatron and the LHC: nonrelativistic-QCD factorization at the crossroads.

    Science.gov (United States)

    Butenschoen, Mathias; Kniehl, Bernd A

    2012-04-27

    We study the polarization observables of J/ψ hadroproduction at next-to-leading order within the factorization formalism of nonrelativistic quantum chromodynamics. We complete the present knowledge of the relativistic corrections by also providing the contribution due to the intermediate (3)P(J)([8]) color-octet states at this order, which turns out to be quite significant. Exploiting the color-octet long-distance matrix elements previously extracted through a global fit to experimental data of unpolarized J/ψ production, we provide theoretical predictions in the helicity and Collins-Soper frames and compare them with data taken by CDF at Fermilab Tevatron I and II and by ALICE at CERN LHC. The notorious CDF J/ψ polarization anomaly familiar from leading-order analyses persists at the quantum level, while the situation looks promising for the LHC, which is bound to bring final clarification.

  5. Measurement of the inclusive isolated prompt photon production cross section at the Tevatron using the CDF detector

    Energy Technology Data Exchange (ETDEWEB)

    Deluca Silberberg, Carolina [Autonomous Univ. of Barcelona (Spain)

    2009-04-01

    In this thesis we present the measurement of the inclusive isolated prompt photon cross section with a total integrated luminosity of 2.5 fb-1 of data collected with the CDF Run II detector at the Fermilab Tevatron Collider. The prompt photon cross section is a classic measurement to test perturbative QCD (pQCD) with potential to provide information on the parton distribution function (PDF), and sensitive to the presence of new physics at large photon transverse momentum. Prompt photons also constitute an irreducible background for important searches such as H → γγ, or SUSY and extra-dimensions with energetic photons in the final state. The Tevatron at Fermilab (Batavia, U.S.A.) is currently the hadron collider that operates at the highest energies in the world. It collides protons and antiprotons with a center-of-mass energy of 1.96 TeV. The CDF and the D0 experiments are located in two of its four interaction regions. In Run I at the Tevatron, the direct photon production cross section was measured by both CDF and DO, and first results in Run II have been presented by the DO Collaboration based on 380 pb-1. Both Run I and Run II results show agreement with the theoretical predictions except for the low pTγ region, where the observed and predicted shapes are different. Prompt photon production has been also extensively measured at fixed-target experiments in lower pTγ ranges, showing excess of data compared to the theory, particularly at high xT. From an experimental point of view, the study of the direct photon production has several advantages compared to QCD studies using jets. Electromagnetic calorimeters have better energy resolution than hadronic calorimeters, and the systematic uncertainty on the photon absolute energy scale is smaller. Furthermore, the determination of the photon kinematics does not require the use of jet algorithms. However, the measurements using photons

  6. A search for the Higgs boson in the zh channel with the D0 detector at the Fermilab Tevatron collider

    Energy Technology Data Exchange (ETDEWEB)

    Heinmiller, James Matthew [Univ. of Illinois, Chicago, IL (United States)

    2006-01-01

    This analysis describes a search for a standard model Higgs boson produced in association with a Z boson through the decay mode ZH → e+e-b$\\bar{b}$ in p$\\bar{p}$ collisions at √s = 1.96 TeV at the Fermilab Tevatron Collider. The data sample used in this analysis corresponds to 452 pb-1 of integrated luminosity accumulated with the D0 detector. Agreement between data and standard model predictions is observed. A 95% confidence level upper exclusion limit for the σ(p$\\bar{p}$ → ZH) x BR(H → b$\\bar{b}$) channel is set between 3.2-8.2 pb for Higgs masses of 105 to 145 GeV.

  7. First measurements of inclusive W and Z cross sections from run II of the fermilab tevatron collider.

    Science.gov (United States)

    Acosta, D; Affolder, T; Akimoto, T; Albrow, M G; Ambrose, D; Amerio, S; Amidei, D; Anastassov, A; Anikeev, K; Annovi, A; Antos, J; Aoki, M; Apollinari, G; Arisawa, T; Arguin, J-F; Artikov, A; Ashmanskas, W; Attal, A; Azfar, F; Azzi-Bacchetta, P; Bacchetta, N; Bachacou, H; Badgett, W; Barbaro-Galtieri, A; Barker, G J; Barnes, V E; Barnett, B A; Baroiant, S; Barone, M; Bauer, G; Bedeschi, F; Behari, S; Belforte, S; Bellettini, G; Bellinger, J; Benjamin, D; Beretvas, A; Bhatti, A; Binkley, M; Bisello, D; Bishai, M; Blair, R E; Blocker, C; Bloom, K; Blumenfeld, B; Bocci, A; Bodek, A; Bolla, G; Bolshov, A; Booth, P S L; Bortoletto, D; Boudreau, J; Bourov, S; Bromberg, C; Brubaker, E; Budagov, J; Budd, H S; Burkett, K; Busetto, G; Bussey, P; Byrum, K L; Cabrera, S; Calafiura, P; Campanelli, M; Campbell, M; Canepa, A; Casarsa, M; Carlsmith, D; Carron, S; Carosi, R; Cavalli-Sforza, M; Castro, A; Catastini, P; Cauz, D; Cerri, A; Cerri, C; Cerrito, L; Chapman, J; Chen, C; Chen, Y C; Chertok, M; Chiarelli, G; Chlachidze, G; Chlebana, F; Cho, I; Cho, K; Chokheli, D; Chu, M L; Chuang, S; Chung, J Y; Chung, W-H; Chung, Y S; Ciobanu, C I; Ciocci, M A; Clark, A G; Clark, D; Coca, M; Connolly, A; Convery, M; Conway, J; Cooper, B; Cordelli, M; Cortiana, G; Cranshaw, J; Cuevas, J; Culbertson, R; Currat, C; Cyr, D; Dagenhart, D; Da Ronco, S; D'Auria, S; de Barbaro, P; De Cecco, S; De Lentdecker, G; Dell'Agnello, S; Dell'Orso, M; Demers, S; Demortier, L; Deninno, M; De Pedis, D; Derwent, P F; Dionisi, C; Dittmann, J R; Doksus, P; Dominguez, A; Donati, S; Donega, M; Donini, J; D'Onofrio, M; Dorigo, T; Drollinger, V; Ebina, K; Eddy, N; Ely, R; Erbacher, R; Erdmann, M; Errede, D; Errede, S; Eusebi, R; Fang, H-C; Farrington, S; Fedorko, I; Feild, R G; Feindt, M; Fernandez, J P; Ferretti, C; Field, R D; Fiori, I; Flanagan, G; Flaugher, B; Flores-Castillo, L R; Foland, A; Forrester, S; Foster, G W; Franklin, M; Freeman, J; Frisch, H; Fujii, Y; Furic, I; Gajjar, A; Gallas, A; Galyardt, J; Gallinaro, M; Garcia-Sciveres, M; Garfinkel, A F; Gay, C; Gerberich, H; Gerdes, D W; Gerchtein, E; Giagu, S; Giannetti, P; Gibson, A; Gibson, K; Ginsburg, C; Giolo, K; Giordani, M; Giurgiu, G; Glagolev, V; Glenzinski, D; Gold, M; Goldschmidt, N; Goldstein, D; Goldstein, J; Gomez, G; Gomez-Ceballos, G; Goncharov, M; González, O; Gorelov, I; Goshaw, A T; Gotra, Y; Goulianos, K; Gresele, A; Grosso-Pilcher, C; Guenther, M; Guimaraes da Costa, J; Haber, C; Hahn, K; Hahn, S R; Halkiadakis, E; Handler, R; Happacher, F; Hara, K; Hare, M; Harr, R F; Harris, R M; Hartmann, F; Hatakeyama, K; Hauser, J; Hays, C; Hayward, H; Heider, E; Heinemann, B; Heinrich, J; Hennecke, M; Herndon, M; Hill, C; Hirschbuehl, D; Hocker, A; Hoffman, K D; Holloway, A; Hou, S; Houlden, M A; Huffman, B T; Huang, Y; Hughes, R E; Huston, J; Ikado, K; Incandela, J; Introzzi, G; Iori, M; Ishizawa, Y; Issever, C; Ivanov, A; Iwata, Y; Iyutin, B; James, E; Jang, D; Jarrell, J; Jeans, D; Jensen, H; Jeon, E J; Jones, M; Joo, K K; Jun, S; Junk, T; Kamon, T; Kang, J; Karagoz Unel, M; Karchin, P E; Kartal, S; Kato, Y; Kemp, Y; Kephart, R; Kerzel, U; Khotilovich, V; Kilminster, B; Kim, D H; Kim, H S; Kim, J E; Kim, M J; Kim, M S; Kim, S B; Kim, S H; Kim, T H; Kim, Y K; King, B T; Kirby, M; Kirsch, L; Klimenko, S; Knuteson, B; Ko, B R; Kobayashi, H; Koehn, P; Kong, D J; Kondo, K; Konigsberg, J; Kordas, K; Korn, A; Korytov, A; Kotelnikov, K; Kotwal, A V; Kovalev, A; Kraus, J; Kravchenko, I; Kreymer, A; Kroll, J; Kruse, M; Krutelyov, V; Kuhlmann, S E; Kuznetsova, N; Laasanen, A T; Lai, S; Lami, S; Lammel, S; Lancaster, J; Lancaster, M; Lander, R; Lannon, K; Lath, A; Latino, G; Lauhakangas, R; Lazzizzera, I; Le, Y; Lecci, C; Lecompte, T; Lee, J; Lee, J; Lee, S W; Leonardo, N; Leone, S; Lewis, J D; Li, K; Lin, C; Lin, C S; Lindgren, M; Liss, T M; Litvintsev, D O; Liu, T; Liu, Y; Lockyer, N S; Loginov, A; Loreti, M; Loverre, P; Lu, R-S; Lucchesi, D; Lujan, P; Lukens, P; Lyons, L; Lys, J; Lysak, R; Macqueen, D; Madrak, R; Maeshima, K; Maksimovic, P; Malferrari, L; Manca, G; Marginean, R; Martin, M; Martin, A; Martin, V; Martínez, M; Maruyama, T; Matsunaga, H; Mattson, M; Mazzanti, P; McFarland, K S; McGivern, D; McIntyre, P M; McNamara, P; Ncnulty, R; Menzemer, S; Menzione, A; Merkel, P; Mesropian, C; Messina, A; Miao, T; Miladinovic, N; Miller, L; Miller, R; Miller, J S; Miquel, R; Miscetti, S; Mitselmakher, G; Miyamoto, A; Miyazaki, Y; Moggi, N; Mohr, B; Moore, R; Morello, M; Moulik, T; Movilla Fernandez, P A; Mukherjee, A; Mulhearn, M; Muller, T; Mumford, R; Munar, A; Murat, P; Nachtman, J; Nahn, S; Nakamura, I; Nakano, I; Napier, A; Napora, R; Naumov, D; Necula, V; Niell, F; Nielsen, J; Nelson, C; Nelson, T; Neu, C; Neubauer, M S; Newman-Holmes, C; Nicollerat, A-S; Nigmanov, T; Nodulman, L; Norniella, O; Oesterberg, K; Ogawa, T; Oh, S H; Oh, Y D; Ohsugi, T; Okusawa, T; Oldeman, R; Orava, R; Orejudos, W

    2005-03-11

    We report the first measurements of inclusive W and Z cross sections times leptonic branching ratios for pp collisions at square root[s]=1.96 TeV, based on their decays to electrons and muons. The data correspond to an integrated luminosity of 72 pb(-1) recorded with the CDF detector at the Fermilab Tevatron. We test e-mu universality in W decays, and we measure the ratio of leptonic W and Z rates from which the leptonic branching fraction B(W-->lnu) can be extracted as well as an indirect value for the total width of the W and the Cabibbo-Kobayashi-Maskawa matrix element, |V(cs)|.

  8. Probing neutrino mass with multilepton production at the Tevatron in the simplest R-parity violation model

    CERN Document Server

    Magro, M B; Éboli, Oscar J P; Porod, Werner; Restrepo, D A; Valle, José W F

    2003-01-01

    We analyze the production of multileptons in the simplest supergravity model with bilinear violation of R parity at the Fermilab Tevatron. Despite the small R-parity violating couplings needed to generate the neutrino masses indicated by current atmospheric neutrino data, the lightest supersymmetric particle is unstable and can decay inside the detector. This leads to a phenomenology quite distinct from that of the R-parity conserving scenario. We quantify by how much the supersymmetric multilepton signals differ from the R-parity conserving expectations, displaying our results in the $m_0 \\otimes m_{1/2}$ plane. We show that the presence of bilinear R-parity violating interactions enhances the supersymmetric multilepton signals over most of the parameter space, specially at moderate and large $m_0$.

  9. L’importation du marbre de Carrare à la cour de Louis XIV : rivalités des marchands et échecs des compagnies

    Directory of Open Access Journals (Sweden)

    Geneviève Bresc-Bautier

    2012-11-01

    Full Text Available La difficulté d’approvisionnement en marbre statuaire a été un problème récurrent pour la sculpture, sauf évidemment en Italie, lieu d’exploitation de carrières, spécialement de celles de Carrare. La France a cherché à exploiter, difficilement, le marbre des Pyrénées, qui a mauvaise réputation auprès des sculpteurs. Les conditions d’extraction, de transport et de commerce du marbre de Carrare en France sous le règne personnel de Louis XIV seront présentées ici. Vers 1660-1662, une première période voit la concurrence entre deux équipes rivales, l’une, envoyée par Fouquet, est composée de Girardin et de Pierre Puget, et celle de Colbert est dirigée par le marchand toulonnais Jacques Beuf, avec son commis Delamer. Cette dernière équipe réussit à débaucher Puget et va, évidemment, l’emporter. Puis Colbert installe deux autres équipes, officielles celles-ci, qui font tirer du marbre par des sculpteurs français envoyés en mission : Antoine André pour le grand banquier Pierre Formont et Nicolas Ménard pour Jacques Beuf - le premier réussissant à évincer le second. Mais Formont, qui avait fait arrêter son sculpteur André et l’avait remplacé par des Flamands, est évincé en raison de sa religion et meurt peu avant la Révocation de l’édit de Nantes (1685. Parallèlement des artistes génois, le peintre Borzone puis les sculpteurs Solaro père et fils, parviennent à imposer des cargaisons de marbre, de même que Puget continue à se procurer directement du marbre à Carrare et même à en vendre. Louvois, prenant le contre-pied de la politique de Colbert, change le système. Il installe d’abord une seule compagnie des marbres officielle, puis lui retire sa charge pour en protéger une seconde, où se retrouvent les mêmes responsables, Haudiquer de Blancourt et André Lebrun. Cette compagnie s’arrête en 1687 devant les risques de la guerre. Un nouvel épisode se situe durant la période d

  10. A Measurement of the Lifetime of the Lambda_b Baryon with the CDF Detector at the Tevatron Run II

    Energy Technology Data Exchange (ETDEWEB)

    Unverhau, Tatjana Alberta Hanna; /Glasgow U.

    2004-12-01

    In March 2001 the Tevatron accelerator entered its Run II phase, providing colliding proton and anti-proton beams with an unprecedented center-of-mass energy of 1.96 TeV. The Tevatron is currently the only accelerator to produce {Lambda}{sub b} baryons, which provides a unique opportunity to measure the properties of these particles. This thesis presents a measurement of the mean lifetime of the {Lambda}{sub b} baryon in the semileptonic channel {Lambda}{sub b}{sup 0} {yields} {Lambda}{sub c}{sup +} {mu}{sup -} {bar {nu}}{sub {mu}}. In total 186 pb{sup -1} of data were used for this analysis, collected with the CDF detector between February 2002 and September 2003. To select the long-lived events from b-decays, the secondary vertex trigger was utilized. This significant addition to the trigger for Run II allows, for the first time, the selection of events with tracks displaced from the primary interaction vertex at the second trigger level. After the application of selection cuts this trigger sample contains approximately 991 {Lambda}{sub b} candidates. To extract the mean lifetime of {Lambda}{sub b} baryons from this sample, they transverse decay length of the candidates is fitted with an unbinned maximum likelihood fit under the consideration of the missing neutrino momentum and the bias introduced by the secondary vertex trigger. The mean lifetime of the {Lambda}{sub b} is measured to be {tau} = 1.29 {+-} 0.11(stat.) {+-} 0.07(syst.) ps equivalent to a mean decay length of c{tau} = 387 {+-} 33(stat.) {+-} 21 (syst.) {micro}m.

  11. Désirs de gares TGV : du projet des édiles locaux au “désaménagement” du territoire Desire for stations : from local officials’ projects to territorial “displanning”

    Directory of Open Access Journals (Sweden)

    Jean-François Troin

    2012-12-01

    Full Text Available Le TGV a suscité en France, à côté de gares urbaines assez bien insérées en ville, des gares “exurbanisées”, stations de plein champ, créées de toutes pièces et bien souvent à la demande d’élus locaux. Ceux-ci en attendaient de multiples bienfaits dont le développement d’activités auprès de la gare. La plupart de ces attentes n’ont pas été satisfaites. Pourquoi alors existe-t-il toujours un fort “désir de gare” chez des élus locaux, des responsables économiques, voisins d’une ligne à grande vitesse en service ou à construire ? Pourquoi dédaigne-t-on le passage des TGV en gare centrale ? Pourquoi ignore-t-on les connexions TGV/trains régionaux pouvant irriguer en profondeur les territoires ?Nous interrogerons l’image perçue du TGV, les compétitions interurbaines, les rationalités économiques, les conceptions territoriales pour rendre compte de ce “désir de gare” et pour conclure à l’impérieuse nécessité d’un cadrage national des rêves d’une grande partie des édiles français, un peu trop prompts à déménager le territoire à leur profit supposé.The French TGV (High Speed Train, beside urban stations well integrated in the city, created some “out of town” railway stations in the open fields, very often by request of local elected officials. Those officials expected many benefits, particularly the development of activities around the station. Most of these hopes have not been fulfilled. So, why does a strong “desire for a station” still exist among local officials, economy leaders neighbouring a High Speed Line (LGV in operation or to be constructed ? Why is the passing of TGV through central stations so much spurned ? Why are connections between regional trains (TER and high-speed trains (TGV nearly always ignored ?We shall examine the perceived image of TGV, interurban competitions, economic rationality, territorial concepts in order to account for this

  12. Les Nymphes dans les rites du mariage

    OpenAIRE

    2013-01-01

    Le champ du mariage (où l’on rencontre à la fois les Nymphes puissances surnaturelles et les numphai humaines) peut se révéler intéressant pour croiser des données littéraires, archéologiques et épigraphiques sur le culte des Nymphes. Lors des préliminaires, ces puissances peuvent être l’objet des protéléia (sacrifices prénuptiaux) ou être associées avec la loutrophorie et le bain prénuptial. Les Nymphes n’interviennent guère pendant la journée de célébration du mariage, sauf dans des textes ...

  13. Pourfour Du Petit syndrome after interscalene block.

    Science.gov (United States)

    Santhosh, Mysore Chandramouli Basappji; Pai, Rohini B; Rao, Raghavendra P

    2013-04-01

    Interscalene block is commonly associated with reversible ipsilateral phrenic nerve block, recurrent laryngeal nerve block, and cervical sympathetic plexus block, presenting as Horner's syndrome. We report a very rare Pourfour Du Petit syndrome which has a clinical presentation opposite to that of Horner's syndrome in a 24-year-old male who was given interscalene block for open reduction and internal fixation of fracture upper third shaft of left humerus.

  14. Sådan forebygger du faldulykker

    DEFF Research Database (Denmark)

    Evron, Lotte

    2015-01-01

    Bidrag til serien 'Eksperten skriver'. Her gennemgås en kort vejledning til, hvordan man arbejder systematisk med faldforebyggelse. Ved at arbejde systematisk med dine hverdagsobservationer kan du få øje på og reagere på ændringer hos svækkede ældre borgere og på den måde forebygge faldet, før de...

  15. Autour du paradigme d’écotourisme

    Directory of Open Access Journals (Sweden)

    Anne-Laure Transler

    2008-02-01

    Full Text Available L’écotourisme ouvre un cadre conceptuel original qui permet d’envisager des démarches renouvelées de développement à partir des revenus issus de consommations touristiques mieux réfléchies et organisées, susceptibles de soutenir des initiatives de développement local s’inscrivant dans un projet global de développement durable. Variante douce du tourisme, loin du tourisme de masse, le champ de l’écotourisme s’étend aux confins du tourisme de nature, du tourisme culturel et des pratiques scientifiques et sportives de plein air. Une définition de l’écotourisme peut être proposée à partir des six points suivants : 1/ nature et culture, 2/ le bien-être des sociétés hôtes, 3/ des touristes responsables, 4/ la participation des sociétés hôtes, 5/ la durabilité, 6/ l’art de la rencontre.Ecotourism provides an original conceptual framework that enables approaches to development that are better able to provide a more equitable distribution of income, as well as better organized and thought through initiatives which are more likely to promote a holistic sustainable local development. With somewhat less negative impact than normal tourism, considerably less that mass tourism, ecotourism can encompass nature tourism, cultural tourism, scientific exploration, and even outdoor sports... A definition of ecotourism should take into account the following six points: 1/ nature and culture, 2/ the welfare of the host community, tourists acting responsibly, 3/ participation by the local community, 5 / sustainability , 6/ promotion of cultural exchanges

  16. Technostress et autres revers du travail nomade

    NARCIS (Netherlands)

    Popma, J.

    2013-01-01

    L'Internet et l'utilisation des ordinateurs portables, des téléphones mobiles et des tablettes ont accru l'importance du « travail nomade». Ce type de travail, sans contrainte de lieu ni de temps, peut entraîner, d’après ce working paper, une plus grande autonomie et une plus grande flexibilité pour

  17. Pourfour Du Petit syndrome after interscalene block

    Directory of Open Access Journals (Sweden)

    Mysore Chandramouli Basappji Santhosh

    2013-01-01

    Full Text Available Interscalene block is commonly associated with reversible ipsilateral phrenic nerve block, recurrent laryngeal nerve block, and cervical sympathetic plexus block, presenting as Horner′s syndrome. We report a very rare Pourfour Du Petit syndrome which has a clinical presentation opposite to that of Horner′s syndrome in a 24-year-old male who was given interscalene block for open reduction and internal fixation of fracture upper third shaft of left humerus.

  18. Sustainable growth, the DuPont way.

    Science.gov (United States)

    Holliday, C

    2001-09-01

    Like many manufacturers, DuPont traditionally has grown by making more and more "stuff." And its business growth has been proportional to the amount of raw materials and energy used--as well as the resulting waste and emissions from operations. Over the years, though, DuPont became aware that cheap supplies of nonrenewable resources wouldn't be endlessly available and that the earth's ecosystems couldn't indefinitely absorb the waste and emissions of production and consumption. Chad Holliday, chairman and CEO of DuPont, believes strongly in the challenge of sustainable growth and makes the business case for it: By using creativity and scientific knowledge effectively, he says, companies can provide strong returns for shareholders and grow their businesses--while also meeting the human needs of societies around the world and reducing the environmental footprint of their operations and products. In fact, a focus on sustainability can help identify new products, markets, partnerships, and intellectual property and lead to substantial business growth. Holliday describes how DuPont developed a three-pronged strategy to translate the concept of sustainability into nuts-and-bolts business practices. Focusing on integrated science, knowledge intensity, and productivity improvement, the strategy was accompanied by a new way to measure progress quantitatively. Sustainable growth should be viewed not as a program for stepped-up environmental performance but as a comprehensive way of doing business, one that delivers tremendous economic value and opens up new opportunities. Ultimately, companies will find that they can generate substantial business value through sustainability while both enhancing the quality of life around the world and protecting the environment.

  19. Pertinence du dépistage du cancer du col de l'utérus au sein d'un établissement de santé

    OpenAIRE

    Chignier, Pauline

    2014-01-01

    Le dépistage du cancer du col de l'utérus est un enjeu de Santé Publique. Le plan cancer 2014-2019 souligne l'importance de réduire les inégalités face au dépistage et de couvrir 80% de la population cible. L'objectif principal de l'étude était d'évaluer la conformité des pratiques cliniques des professionnels de santé aux recommandations de la HAS. L'objectif secondaire était d'évaluer la qualité du dépistage du cancer du col selon le type de suivi : gynécologique versus obstétrical. Il s'ag...

  20. Rapport d'Activite du Service Medical - 2001/2002

    CERN Document Server

    Fassnacht, V

    2003-01-01

    Le rapport annuel de l’année 2002 fait état de l’activité du service médical et de ses conclusions en matière de santé au travail ou de conditions de travail pour les membres du personnel du CERN, c’est à dire!: les titulaires, boursiers, étudiants, utilisateurs, attachés, etc…