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Sample records for acelerador lineal linac

  1. Dose attenuation by a carbon fiber linac couch and modeling with a treatment planning system; Medida de la atenuacion producida por la mesa de tratamiento de un acelerador lineal y su modelado en un sistema de planificacion

    Sanchez Galiano, P.; Garcia Sancho, J.M.; Crelgo, D.; Pamos, M.; Fernandez, J.; Vivanco, J.

    2010-07-01

    The purpose of this work is to investigate the attenuation caused by a carbon fiber linac treatment couch and the ability of a commercial radiotherapy treatment planning system to simulate it. The attenuation caused by an Exact{copyright} treatment couch in a Varian{copyright} Clinac{copyright} 2100 C/D was characterized in detail. Both 6 MV and 18 MV photon beams were studied. The treatment couch was modeled and incorporated to Elekta{copyright} XiO{copyright} treatment planning system. Measured and computed attenuation values were compared. As a result we found that the attenuation caused by this complex treatment couch is strongly dependent on the incidence angle of the beam. The measured attenuation values reach 16% for 6 MV and 10% for 18 MV. The model incorporated to the treatment planning software allows reducing the differences between measured and calculated data below 2.5% and 2.0% for 6 MV and 18 MV respectively. In conclusion, it is strongly recommended accounting for the perturbation caused by this carbon fiber treatment couch when the beam intersects it. The treatment planning system studied can simulate this treatment couch accurately. Clinical implementation of the described method requires a reliable procedure to reproduce the same patient geometry in the treatment delivery and planning. (Author).

  2. Dose around a lineal accelerator of medical use;Dosis en torno a un acelerador lineal de uso medico

    Hernandez A, B.; Ortiz H, A.; Hernandez D, V. M.; Vega C, H. R. [Universidad Autonoma de Zacatecas, Unidad Academica de Estudios Nucleares, Calle Cipres No. 10, Fracc. La Penuela, 98068 Zacatecas (Mexico); Rivera M, T. [IPN, Centro de Investigacion en Ciencia Aplicada y Tecnologia Avanzada, Av. Legaria 694, 11500 Mexico D. F. (Mexico); Azorin N, J., E-mail: ice_bere_nice@hotmail.co [Universidad Autonoma Metropolitana, Unidad Iztapalapa, Av. San Rafael Atlixco 186, 09340 Mexico D. F. (Mexico)

    2009-10-15

    By means of a measures series the dosimetric characteristics of the photo neutrons that take place around a lineal accelerator of radiotherapy of 18 MV has been determinate, this it is a linac Varian model 21EX Platinum Plus. The neutron spectrum was established to 100 cm of the isocenter, when it is locates to 10 cm inside an equivalent water phantom. The spectrum was measured with a spectrometric system of Bonner spheres, the used spheres were of 0, 2, 3, 5, 8, 10 and 12 inches of diameter. In the spheres center they were inserted pairs of thermoluminescent dosemeters of the type 600 and 700 as thermal neutrons detector. The due net signal to the neutrons measured with each sphere was used to reconstruct the neutron spectrum; this reconstruction was made with the BUNKIUT code and the response matrix UTA4. The phantom isocenter was exposed at 600 U M and during the irradiation process the rates of environmental equivalent dose were measured by neutrons and photons on the control area of the accelerator. Immediately after having applied the 600 U M the rate of environmental equivalent dose it was measured inside the enclosure and in points around the stretcher due to the neutronic activation. The measured spectrum presents two maxima, one in the thermal neutrons area and the other between 0.1 and 1 MeV, this spectrum is similar to those reported in the literature. The thermal neutrons are produced mainly the {sup r}oom return{sup ,} while the neutrons of approximately 0.5 MeV are those transmitted through the linac head stock. The dose rates in the control area of the accelerator are 3.1 and 0.93 muSv-h{sup -1} for photons and neutrons respectively. Around the stretcher the rates of due dose to the activation photons vary from 6 to 26.1 muSv-h{sup -1}, depending on the measurement place. (Author)

  3. Procedure to measure the neutrons spectrum around a lineal accelerator for radiotherapy; Procedimiento para medir el espectro de los neutrones en torno a un acelerador lineal para radioterapia

    Vega C, H. R.; Hernandez D, V. M.; Letechipia de L, C. [Universidad Autonoma de Zacatecas, Unidad Academica de Estudios Nucleares, Cipres No. 10, Fracc. La Penuela, 98060 Zacatecas (Mexico); Benites R, J. L. [Servicios de Salud de Nayarit, Centro Estatal de Cancerologia, Calzada de la Cruz 116 Sur, 63000 Tepic, Nayarit (Mexico); Salas L, M. A., E-mail: fermineutron@yahoo.com [Universidad Autonoma de Zacatecas, Unidad Academica de Agronomia, Apdo. Postal 336, 98000 Zacatecas (Mexico)

    2013-10-15

    An experimental procedure was developed, by means of Bonner spheres, to measure the neutrons spectrum around Linacs of medical use that only requires of a single shot of the accelerator; to this procedure we denominate Planetary or Isocentric method. One of the problems associated to the neutrons spectrum measurement in a radiotherapy room with lineal accelerator is because inside the room a mixed, intense and pulsed radiation field takes place affecting the detection systems based on active detector; this situation is solved using a passive detector. In the case of the Bonner spheres spectrometer the active detector has been substituted by activation detectors, trace detectors or thermoluminescent dosimeters. This spectrometer uses several spheres that are situated one at a time in the measurement point, this way to have the complete measurements group the accelerator should be operated, under the same conditions, so many times like spheres have the spectrometer, this activity can consume a long time and in occasions due to the work load of Linac to complicate the measurement process too. The procedure developed in this work consisted on to situate all the spectrometer spheres at the same time and to make the reading by means of a single shot, to be able to apply this procedure, is necessary that before the measurements two characteristics are evaluated: the cross-talking of the spheres and the symmetry conditions of the neutron field. This method has been applied to determine the photo-neutrons spectrum produced by a lineal accelerator of medical use Varian ix of 15 MV to 100 cm of the isocenter located to 5 cm of depth of a solid water mannequin of 30 x 30 x 15 cm. The spectrum was used to determine the total flow and the environmental dose equivalent. (Author)

  4. Planetary method to measure the neutrons spectrum in lineal accelerators of medical use; Metodo planetario para medir el espectro de neutrones en aceleradores lineales de uso medico

    Vega C, H. R. [Universidad Autonoma de Zacatecas, Unidad Academica de Estudios Nucleares, Cipres No. 10, Fracc. La Penuela, 98068 Zacatecas (Mexico); Benites R, J. L., E-mail: fermineutron@yahoo.com [Centro Estatal de Cancerologia de Nayarit, Servicio de Seguridad Radiologica, Calzada de la Cruz 118 Sur, 63000 Tepic, Nayarit (Mexico)

    2014-08-15

    A novel procedure to measure the neutrons spectrum originated in a lineal accelerator of medical use has been developed. The method uses a passive spectrometer of Bonner spheres. The main advantage of the method is that only requires of a single shot of the accelerator. When this is used around a lineal accelerator is necessary to operate it under the same conditions so many times like the spheres that contain the spectrometer, activity that consumes enough time. The developed procedure consists on situating all the spheres of the spectrometer at the same time and to realize the reading making a single shot. With this method the photo neutrons spectrum produced by a lineal accelerator Varian ix of 15 MV to 100 cm of the isocenter was determined, with the spectrum is determined the total flow and the ambient dose equivalent. (Author)

  5. Optimizacion de una linea de espectrometria neutronica de transmision aplicada a ciencia de materiales para el acelerador lineal del CAB

    The Neutrons and Reactors Laboratory (NYR) of CAB (Centro Atomico Bariloche) is equipped with a linear electron accelerator (LINAC) Linear particle accelerator). This LINAC is used as a neutron source from which two beams are extracted to perform neutron transmission and dispersion experiments. Through these experiments, structural and dynamic properties of materials can be studied. The neutron transmission experiments consist in a collimated neutron beam which interacts with a sample and a detector behind the sample. Important information about the microstructural characteristics of the material can be obtained from the comparison between neutron spectra before and after the interaction with the sample. This experimental technique has been extensively used to determine cross sections, lattice parameters of a crystalline solid, vibration frequencies of atoms or the strain field of a material. In the NYR Laboratory, cylindrical samples of one inch of diameter have been traditionally studied. Nonetheless, there is a great motivation for doing systematic research on smaller and with different geometries samples; particularly sheets and samples for tensile tests. In such cases, a reduction of the spot size of the beam and an increase of its intensity would have a direct impact on minimizing measurement times. Hence, in the NYR Laboratory it has been considered the possibility of incorporating a neutron guide into the existent transmission line. According to all mentioned above, the main objective of this work consisted in the optimization of the flight transmission tube optics of neutrons. This optimization not only improved the existent line but also contributed to an election criterion for the neutron guide acquisition. The optimization was directed towards maximize the neutron flux on samples of mentioned geometries and to form the divergence of the incident beam upon them. It was then necessary to study the instrument neutron optics, i.e. the characteristics of the

  6. Dosimetry of the energy of the electrons beam and virtual distance of the source of a lineal accelerator; Dosimetria de la energia del haz de electrones y distancia virtual de la fuente de un acelerador lineal

    Gonzales, A.; Garcia, B.; Ramirez, J.; Marquina, J., E-mail: andres.gonzales@aliada.com.pe [ALIADA, Oncologia Integral, Av. Jose Galvez Barrenechea 1044, San Isidro, Lima 27 (Peru)

    2014-08-15

    The objectives of this work were to characterize, to gauge the energy of a electrons beam of 12 MeV and to find the virtual distance of the source for a lineal accelerator Trilogy-Varian. For the characterization, calibration and to find the virtual distance of the source of a lineal accelerator Trilogy-Varian, a water phantom was used (cylindrical Cuba 3-D) of Sun-Nuclear. The following values were found: R{sub 50.ion} = 4, 95 g/cm{sup 2}, R{sub 50} = 5, 04 g/cm{sup 2}, Z{sub ref} = 2,92 g/cm{sup 2}, Z{sub max} = 2, 60 g/cm{sup 2}. In the calibration was found D{sub W,Q}(Z{sub max}) = 1, 0015 c Gy/Um. In the profile In-plane was measured a symmetry and flatness of 1, 9% and 1, 6% respectively. In the profile Cross-plane a symmetry was measured and flatness of 1, 9% and 1, 3% respectively. The virtual distance regarding the source was of DFS (virtual) =105,81 cm. The electrons beam of 12 MeV was characterized and gauged satisfactorily, were carried out the In-plane and Cross-plane profiles, obtaining all the parameters inside the acceptance limit. The virtual distance of the source was of 105,81 cm. (Author)

  7. La falta de financiacion publica hipoteca el futuro del acelerador de protones valenciano. La Universidad de Valencia tiene avanzado el diseno de este dispositivo de alta tecnologia

    Jatvia, J M

    2002-01-01

    "La Universidad de Valencia tiene avanzado el diseno de un acelerador lineal de protones, cuya culminacion depende del compromiso del Consell en sufragar la plantilla que necesitaria el centro para estar operativo" (1 page).

  8. Determination of the neutron spectra in the treatment room of a linear accelerator for radiotherapy; Determinacion de los espectros de neutrones en la sala de tratamiento de un acelerador lineal para radioterapia

    Vega C, H.R. [Universidad Autonoma de Zacatecas, Cuerpo Academico de Radiobiologia, A.P. 336, 98000 Zacatecas (Mexico); Barquero, R. [Hospital Universitario Rio Hortega, Valladolid (Spain); Mendez, R.; Iniguez, M.P. [Depto. de Fisica Teorica, Atomica, Molecular y Nuclear, Universidad de Valladolid, 47011 Valladolid (Spain)

    2003-07-01

    By means of a series of measures and Monte Carlo calculations the dosimetric characteristics of the photoneutrons have been determined that take place in volume to a linear accelerator of radiotherapy of 18 MV, LINAC, mark Siemens Mevatron model. The measures were carried out with thermoluminescent dosemeters TLD 600 and TLD 700 that were naked exposed and confined with cover of Cd and Sn, inside a sphere of paraffin and inside spheres Bonner. (Author)

  9. Measurement of the dose by dispersed radiation in a lineal accelerator using thermoluminescent dosimeters of CaSO{sub 4}:Dy; Medicion de la dosis por radiacion dispersa en un acelerador lineal usando dosimetros termoluminiscentes de CaSO{sub 4}:Dy

    Chavez C, N.; Torijano, E.; Azorin, J. [Universidad Autonoma Metropolitana, Unidad Iztapalapa, Av. San Rafael Atlixco 186, Col. Vicentina, 09340 Mexico D. F. (Mexico); Herrera, A. [ISSSTE, Hospital Nacional 20 de Noviembre, Eje 7 Sur Felix Cuevas Esq. Av. Coyoacan, Col. del Valle, 03229 Mexico D. F. (Mexico)

    2014-08-15

    The thermoluminescence (Tl) is based on the principle of the luminescent in a material when is heated below their incandescence temperature. Is a technique very used in dosimetry that is based on the property that have most of the crystalline materials regarding the storage of the energy that they absorb when are exposed to the ionizing radiations. When this material has been irradiated previously, the radioactive energy that contains is liberated in form of light. In general, the principles that govern the thermoluminescence are in essence the same of those responsible for all the luminescent processes and, this way, the thermoluminescence is one of the processes that are part of the luminescence phenomenon. For this work, the dispersed radiation was measured in the therapy area of the lineal accelerator of medical use type Elekta, using thermoluminescent dosimeters of CaSO{sub 4}:Dy + Ptfe developed and elaborated in the Universidad Autonoma Metropolitana, Unidad Iztapalapa. With the dosimeters already characterized and calibrated, we proceeded to measure the dispersed radiation being a patient in treatment. The results showed values for the dispersed radiation the order of a third of the dose received by the patient on the treatment table at 30 cm of the direct beam and the order of a hundredth in the control area (4 m of the direct beam, approximately). The conclusion is that the thermoluminescent dosimeters of CaSO{sub 4}: Dy + Ptfe are appropriate to measure dispersed radiation dose in radiotherapy. (author)

  10. Sistema de Planificación de Tratamientos de Radioterapia para Aceleradores Lineales de Partículas (LinAc) basado en el método Monte Carlo

    ABELLA ARANDA, VICENTE

    2014-01-01

    La principal motivación que ha propiciado el veloz progreso de las técnicas de prevención y tratamiento del cáncer en los últimos años ha sido, y continúa siendo, su protagonismo en las listas de principales causas de muerte: más de 10 millones de diagnósticos anuales a escala global y más de 160.000 en territorio español. En este contexto, la implementación clínica de los Sistemas de Planificación de Tratamientos de Radioterapia (RTPS) ha desempeñado un papel capital. Resulta lugar comú...

  11. Reconstruction of the Bremsstrahlung spectrum a medical linear accelerator from the gradient of the depth dose curve in a water container; Reconstruccion del espectro Bremsstrahlung emitido por un acelerador lineal medico a partir del gradiente de las curvas de dosisen profundidad en una cuba de agua

    Juste, B.; Miro, R.; Verdu, G.; Diez, S.; Campayo, J. M.

    2010-07-01

    Determining the spectral distribution of the emitted photon medical linear accelerator (linac) used in radiotherapy treatment is extremely important for performing dosimetry calculations as to accurately calculate the therapeutic dose distributions. Since directly measure the spectrum is very complicated, this paper presents an indirect technique to accurately calculate the spectra of Bremsstrahlung photons emitted by linacs.

  12. Dosimetric comparison on tissue interfaces with TLD dosimeters, L-alanine, EDR2 films and Penelope simulation for a Co-60 source and linear accelerator in radiotherapy; Comparacion dosimetrica en interfaces de tejidos con dosimetros TLD, L-alanina, peliculas EDR2 y simulacion Penelope para una fuente de Co-60 y acelerador lineal en radioterapia

    Vega R, J. L.; Cayllahua, F.; Apaza, D. G.; Javier, H., E-mail: josevegaramirez@yahoo.es [Universidad Nacional de San Agustin, Departamento de Fisica, Av. Independencia s/n, Arequipa (Peru)

    2015-10-15

    Percentage depth dose curves were obtained with TLD-100 dosimeters, EDR2 films and Penelope simulation at the interfaces in an inhomogeneous mannequin, composed by equivalent materials to the human body built for this study, consisting of cylindrical plates of solid water-bone-lung-bone-solid water of 15 cm in diameter and 1 cm in height; plates were placed in descending way (4-2-8-2-4). Irradiated with Co-60 source (Theratron Equinox-100) for small radiation fields 3 x 3 cm{sup 2} and 1 x 1 cm{sup 2} at a surface source distance of 100 cm from mannequin. The TLD-100 dosimeters were placed in the center of each plate of mannequin irradiated at 10 Gy. The results were compared between these measurement techniques, giving good agreement in interfaces better than 97%. This study was compared with the same characteristics of another study realized with other equivalent materials to human body not homogeneous acrylic-bone-cork-bone-acrylic. The percentage depth dose curves were obtained with mini-dosimeters L-alanine of 1 mm in diameter and 3 mm in height and 3.5 to 4.0 mg of mass with spectrometer band K (EPR). The mini-dosimeters were irradiated with a lineal accelerator PRIMUS Siemens 6 MV. The results of percentage depth dose of L-alanine mini-dosimeters show a good agreement with the percentage depth dose curves of Penelope code, better than 97.7% in interfaces of tissues. (Author)

  13. Aplicación del Método de Monte Carlo a la Planificación en Radioterapia y a la Reconstrucción de Espectros de Fotones de Aceleradores Lineales de Partículas (LinAc)

    Juste Vidal, Belen Jeanine

    2011-01-01

    La radioterapia es uno de los tratamientos más generalizados aplicados a los pacientes que padecen determinados tipos de cáncer. Sin embargo, la efectividad de este tipo de tratamientos en la destrucción de las células cancerígenas lleva asociada la posibilidad de sufrir los efectos secundarios de la radiación sobre los tejidos sanos circundantes. El riesgo de lesión de las células sanas depende fundamentalmente de la orientación del haz emitido por la unidad de radioterapia y de la intensida...

  14. Un ano de retraso para el acelerador europeo LHC

    CERN. Geneva

    2002-01-01

    "Debido a las dificultades presupuestarias que sufre el Laboratorio Europeo de Fisica de Particulas (CERN) para construir el nuevo acelerador LHC, la puesta en marcha de esta gran instalacion se retrasara un ano, entrando en funcionamiento en 2007, segun el plan elaborado por la direccion del centro" (1/2 page).

  15. LINAC 4

    2013-01-01

    On 13 March, a beam of negative hydrogen ions was injected into the first accelerator module of Linac 4, the linear accelerator which will replace Linac 2. The beam was created in the new source built for Linac 4 and accelerated from 45 kEV to 3 MeV by a radiofrequency quadrupole (RFQ) module, the first link in the Linac 4 accelerator chain. This crucial phase went off without a hitch. The video above shows the new Linac 4 ion source, the low-energy transfer line and the RFQ, with running commentary by Giulia Bellodi and Carlo Rossi from the Beams Department.

  16. Ajuste lineal mediante Microsoft Excel

    Borrás Falomir, Luis; Martí Ortega, Nuria

    2013-01-01

    En este vídeo se muestra cómo utilizar la hoja de cálculo Excel de Microsoft para realizar un ajuste lineal de una serie de puntos. El vídeo detalla cómo obtener los parámetros de la ecuación lineal gráficamente y utilizando las funciones predefinidas de Excel, desarrollado para el Proyecto de Innovación Educativa Innovación Docente en Ingeniería Química (IDIQ).

  17. Superconducting linac

    This project has two goals: to design, build, and test a small superconducting linac to serve as an energy booster for heavy ions from an FN tandem electrostatic accelerator, and to investigate various aspects of superconducting rf technology. The main design features of the booster are described, a status report on various components (resonators, rf control system, linac control system, cryostats, buncher) is given, and plans for the near future are outlined. Investigations of superconducting-linac technology concern studies on materials and fabrication techniques, resonator diagnostic techniques, rf-phase control, beam dynamics computer programs, asymmetry in accelerating field, and surface-treatment techniques. The overall layout of the to-be-proposed ATLAS, the Argonne Tandem-Linac Accelerator System, is shown; the ATLAS would use superconducting technology to produce beams of 5 to 25 MeV/A. 6 figures

  18. Demo 89. Acelerador magnético o de Gauss

    Ferrer Roca, Chantal; Cros Stotter, Ana

    2013-01-01

    Objetivo: Entender un fenómeno de aparente no conservación de la energía y momento lineal. Profundizar en el concepto de energía de ligadura y energía interna y su relación con la energía cinética.

  19. Dose around a lineal accelerator of medical use

    By means of a measures series the dosimetric characteristics of the photo neutrons that take place around a lineal accelerator of radiotherapy of 18 MV has been determinate, this it is a linac Varian model 21EX Platinum Plus. The neutron spectrum was established to 100 cm of the isocenter, when it is locates to 10 cm inside an equivalent water phantom. The spectrum was measured with a spectrometric system of Bonner spheres, the used spheres were of 0, 2, 3, 5, 8, 10 and 12 inches of diameter. In the spheres center they were inserted pairs of thermoluminescent dosemeters of the type 600 and 700 as thermal neutrons detector. The due net signal to the neutrons measured with each sphere was used to reconstruct the neutron spectrum; this reconstruction was made with the BUNKIUT code and the response matrix UTA4. The phantom isocenter was exposed at 600 U M and during the irradiation process the rates of environmental equivalent dose were measured by neutrons and photons on the control area of the accelerator. Immediately after having applied the 600 U M the rate of environmental equivalent dose it was measured inside the enclosure and in points around the stretcher due to the neutronic activation. The measured spectrum presents two maxima, one in the thermal neutrons area and the other between 0.1 and 1 MeV, this spectrum is similar to those reported in the literature. The thermal neutrons are produced mainly the room return, while the neutrons of approximately 0.5 MeV are those transmitted through the linac head stock. The dose rates in the control area of the accelerator are 3.1 and 0.93 μSv-h-1 for photons and neutrons respectively. Around the stretcher the rates of due dose to the activation photons vary from 6 to 26.1 μSv-h-1, depending on the measurement place. (Author)

  20. Linear Accelerator (LINAC)

    ... News Physician Resources Professions Site Index A-Z Linear Accelerator A linear accelerator (LINAC) customizes high energy x-rays to ... ensured? What is this equipment used for? A linear accelerator (LINAC) is the device most commonly used ...

  1. A special fermionic generalization of lineal gravity

    2006-01-01

    The central extension of the (1+1)-dimensional Poincaré algebra by including fermionic charges which obey not supersymmetric algebra, but a special graded algebra containing in the right hand side a central element only is obtained. The corresponding theory being the fermionic extension of the lineal gravity is proposed. We considered the algebra of generators, the field transformations and found Lagrangian and equation of motion, then we derived the Casimir operator and obtained the constant black hole mass.

  2. Circuitos y sistemas lineales : curso de laboratorio

    Bertran Albertí, Eduardo; Montoro López, Gabriel

    2000-01-01

    Este curso se ha diseñado para una asignatura de Circuitos y Sistemas Lineales que tenga el objetivo de dar unos fundamentos teóricos contrastados con trabajos experimentales. Cada práctica de laboratorio está compuesta por tres apartados: bases, estudio previo y trabajo de laboratorio. El objetivo de las bases es dar una información previa al trabajo experimental de forma que el alumno tenga los fundamentos necesarios para saber qué va a hacer y porqué va a hacerlo. El estudio previo es un c...

  3. Linear concentration system; Sistema de concentracion lineal

    Gonzalez Lugo, J.I; Leon Rovira, N; Aguayo Tellez, H [Instituto Tecnologico y de Estudios Superiores de Monterrey, Monterrey, Nuevo Leon (Mexico)]. E-mails: a00812662@itesm.mx; noel.leon@itesm.mx; haguayo@itesm.mx

    2013-03-15

    Solar linear concentration technologies to generate high temperatures are limited to the ranges of 200 to 500 degrees Celsius. While its performance has been tested through prototypes and pilot plants around the world, there are still areas of opportunity that can be exploited to obtain a linear concentration that achieves temperatures above this range in order to have a better use of the available solar energy. Because of this: It is possible to develop a linear concentration system that can track the sun with minimal movement of the absorber-receiver while maintaining temperatures above 850 degrees Celsius sufficient for industrial processes that require that temperature. The methodology consists of a series of stages (conceptual design, simulation, evaluation, development concept, results and validation) through which concepts are generated that allow design and evaluation of solar concentrator configurations with the help of simulation software. We have designed a linear parabolic concentrating system which comprises a set of mirrors segments with different focal lengths that works within the range of 600 degrees Celsius; however, it is advancing in the development of a double concentration to reach 850 degrees Celsius. [Spanish] Las tecnologias de concentracion lineal solar para generar altas temperaturas se ven limitadas a los rangos de 200 a 500 grados centigrados. Si bien su funcionamiento ha sido probado a traves de prototipos y plantas piloto alrededor del mundo, aun existen areas de oportunidad que pueden ser aprovechadas para obtener un sistema de concentracion lineal que permita alcanzar temperaturas mayores a este rango para asi tener un mejor aprovechamiento de la energia solar disponible. Debido a esto: Es posible desarrollar un sistema de concentracion lineal capaz de seguir la trayectoria del Sol con minimo movimiento del absorbedor-recibidor al mismo tiempo que mantiene temperaturas superiores a los 850 grados centigrados suficientes para

  4. Programación lineal y diccionarios

    González, Martín; Herrera, G

    2002-01-01

    Por la importancia que tiene, por las aplicaciones prácticas y por su sencillez, dentro de los contenidos básicos de las matemáticas de bachillerato sería obligado incluir una introducción a la programación lineal. Actualmente, dichos contenidos sólo se imparten en los bachilleratos de ciencias sociales, resolviendo algunos problemas sencillos con la ayuda del método gráfico. En este trabajo se propone un método alternativo consistente en la utilización de una herramienta sencilla y eficaz (l...

  5. Procedure to measure the neutrons spectrum around a lineal accelerator for radiotherapy

    An experimental procedure was developed, by means of Bonner spheres, to measure the neutrons spectrum around Linacs of medical use that only requires of a single shot of the accelerator; to this procedure we denominate Planetary or Isocentric method. One of the problems associated to the neutrons spectrum measurement in a radiotherapy room with lineal accelerator is because inside the room a mixed, intense and pulsed radiation field takes place affecting the detection systems based on active detector; this situation is solved using a passive detector. In the case of the Bonner spheres spectrometer the active detector has been substituted by activation detectors, trace detectors or thermoluminescent dosimeters. This spectrometer uses several spheres that are situated one at a time in the measurement point, this way to have the complete measurements group the accelerator should be operated, under the same conditions, so many times like spheres have the spectrometer, this activity can consume a long time and in occasions due to the work load of Linac to complicate the measurement process too. The procedure developed in this work consisted on to situate all the spectrometer spheres at the same time and to make the reading by means of a single shot, to be able to apply this procedure, is necessary that before the measurements two characteristics are evaluated: the cross-talking of the spheres and the symmetry conditions of the neutron field. This method has been applied to determine the photo-neutrons spectrum produced by a lineal accelerator of medical use Varian ix of 15 MV to 100 cm of the isocenter located to 5 cm of depth of a solid water mannequin of 30 x 30 x 15 cm. The spectrum was used to determine the total flow and the environmental dose equivalent. (Author)

  6. Linac working group technical summary

    The working group looked at linac injectors for a Superconducting Super Collider (SSC) or Hadron Facility. Discussion includes rf power, a possible strawman linac, ion source/injector, radio-frequency quadrupole, and coupled-cavity linac

  7. Linac 1, inner structure

    1968-01-01

    This photo shows the inner structure of Linac 1. As injector to the PS, and later to the Booster, Linac 1 accelerated protons to 50 MeV, but it has also accelerated heavier ions. Fitted with a 520 keV RFQ pre-injector (instead of the original Cockcroft-Walton generator), it delivered protons and heavy ions to LEAR, from 1982 to 1992. After 33 years of faithful service, Linac 1 was dismantled in 1992 to make room for Linac 3 (Pb ions).

  8. Álgebra lineal y geometría I, 2010-11

    Serrano Sotelo, Gloria; Hernádez Serrano, Daniel; Sánchez Gómez, Darío

    2010-01-01

    I. Materiales de clase: Tema 1. Espacios y subespacios vectoriales. Dependencia e indepencia lineal. Bases y dimensión; Tema 2. Operaciones con subespacios. Subespacios suplementarios; Tema 3. Aplicaciones lineales. Núcleo e imagen de una aplicación lineal. Tipos de aplicaciones lineales; Tema 4. Aplicaciones lineales en coordenadas: matrices. Sistemas lineales. Cambios de base; Tema 5. Funciones coordenadas. Espacio dual. Subespacio incidente. Ecuaciones paramétricas e implícitas de un subes...

  9. Workshop: Linac90

    In 1960 the first linear accelerator (linac) conference was organized at Brookhaven by John Blewett. In the few years following, linear accelerator energies jumped from 50 MeV (at Brookhaven and CERN) to 2 GeV at Stanford. With the realization that, at least for electrons, circular accelerators have reached their practical limits, linacs are once more in the spotlight

  10. Linac pre-injector

    1965-01-01

    New accelerating column of the linac pre-injector, supporting frame and pumping system. This new system uses two mercury diffusion pumps (in the centre) and forms part of the modifications intended to increase the intensity of the linac. View taken during assembly in the workshop.

  11. High-gradient accelerating structure studies and their application in hadrontherapy

    Verdú Andrés, S.

    2013-01-01

    Este proyecto de tesis doctoral tiene como objetivo el estudio de las cavidades de aceleración de alto gradiente y su aplicación al campo de la hadronterapia, en particular, al desarrollo de un acelerador lineal (linac) para hadronterapia. Las reducidas dimensiones de los linacs que usan estructuras de Radio-Frecuencia (RF) de alto gradiente contribuyen a su menor coste y los hacen muy atractivos para su aplicación en una amplia variedad de campos, d...

  12. The Linac4 Project

    Lombardi, Alessandra

    2016-01-01

    Linac4 is a normal conducting, 160 MeV H- ion accelerator that is being constructed within the scope of the LHC injectors upgrade project. Linac4 will be connected to the Proton Synchrotron Booster (PSB) during the next long LHC shut-down and it will replace the current 50 MeV hadron linac, Linac2. Linac4 is presently being commissioned, with the aim of achieving the final energy at the end of the year. A test of the injection chicane and a reliability run will follow. The beam commissioning, in steps of increasing energy, has been prepared by an extended series of studies and interlaced with phases of installation. In this paper we will detail the beam dynamics challenges and we will report on the commissioning results.

  13. Consideraciones generales acerca de la lógica lineal

    Nunes de Medeiros, Maria da Paz; Universidade Federal de Rio Grande do Norte

    2013-01-01

    En este trabajo se hacen consideraciones generales acerca de la lógica lineal, tomando especialmente en cuenta sus motivaciones y su formalización. En primer lugar, se explica la necesidad de expandir el conjunto usual de conectivas lógicas en la lógica lineal. Siguiendo a Girard (1987), se presenta una formalización para la lógica lineal como un cálculo de secuentes y se esboza el teorema de eliminación de corte para este sistema. Finalmente, se lleva a cabo un análisis crítico de la traducc...

  14. Estudio in vitro de la supervivencia en células tumorales irradiadas con un acelerador lineal de uso clínico

    Quintero Mejía, Paulo Alejandro

    2012-01-01

    El Trabajo Final de Maestría en Física Médica presentado es un estudio sobre el efecto de las radiaciones ionizantes en células cancerígenas de colon y cérvix en función de la supervivencia celular. Contó con la participación y apoyo del grupo de investigación de Física Médica de la Universidad Nacional de Colombia, el grupo BIO-BIO de Bioquímica de la Universidad del Rosario y el grupo de Física Médica del Instituto Nacional de Cancerología E.S.E. El objetivo principal fue estudiar en condic...

  15. A model for the determination of the nominal potential for a linear accelerator; Un modelo para la determinacion del potencial nominal de un acelerador lineal

    Gutt, F.; Silva, P.; Guerrero, R.; Diaz, J.; Colmenares, J. [Instituto Venezolano de Investigaciones Cientificas (IVIC), Laboratorio Secundario de Calibracion Dosimetrica (LSCD), Apartado 21827, Caracas 1020 A (Venezuela)

    1998-12-31

    The objective of the present work is to find a physical mathematical model based on the reason of the dose percentages at 10 and 20 cm depth, at 100 cm DFS and a 10 x 10 cm{sup 2} field. It was utilized literature data of new manufactured accelerators and those are in use in hospitals, which allow to prove the model under different conditions. Our objective consists only to obtain a model that verifies the nominal potential for a linear accelerator, but without pretending that such a model to be used to calculate any one factor to determination of absorbed dose. (Author)

  16. Periodic quality control of a linear accelerator using electronic portal imaging; Controles de calidad periodicos de un acelerador lineal utilizando el sistema electronico de imagenes portales

    Planes Meseguer, D.; Dorado Rodriguez, M. P.; Esposito, R. D.

    2011-07-01

    In this paper we present our solution for the realization of the monthly periodic quality control (CP) geometry - mechanical and multi leaf collimator (MLC), using the electronic system for portal imaging (EPI). We have developed specific programs created with free software. The monitoring results are automatically stored on our web server, along with other information generated in our service.

  17. Pulsed SC Proton Linac

    Ouchi, N.; Chishiro, E.; Tsukishima, C.; Mukugi, K.

    2000-01-01

    The superconducting (SC) proton linac is proposed in the JAERI/KEK Joint Project for a high-intensity proton accelerator in the energy region from 400 to 600 MeV. Highly stable fields in the SC cavities are required under the dynamic Lorentz force detuning. A new model describing the dynamic Lorentz detuning has been developed and the validity has been confirmed experimentally. The model has been applied successfully to the rf control simulation of the SC proton linac.

  18. Assessment of the factors field for fields small of a throttle lineal multienergetic by diodes and radiochromic film; Evaluacion de los factores campo pra campos pequalos de un acelerador lineal multienergetico mediante diodos y pelicul radiocromica

    Ramirez-Ros, J.; Garcia-Marcos, R.; Huertas Martinez, M. c.; Hurtado Sanchez, A.

    2015-07-01

    We discuss the field factors obtained for a linear accelerator electron multi energetic with irradiation standard modes and flatter unfiltered. We compared the values obtained with several diodes, two chambers of ionization and film radiochromic We obtain correction factors for diodes and. Finally, we evaluate the Daisy-Chain method, depending on the detector and the field of step. (Author)

  19. Comportamiento lineal y no lineal de las deflexiones en vigas de concreto reforzado

    Wilmer Alfredo Martínez Maldonado, Oscar Javier Gutiérrez Junco

    2011-05-01

    Full Text Available El  objetivo  del  trabajo  que  aquí  se  presenta  fue determinar el comportamiento lineal y no lineal de las deflexiones en vigas de concreto reforzado, producidas por la aplicación de una carga puntual en el centro de la  luz, y comparar los comportamientos hasta y más allá  del  estado  elástico,  con  base  en modelosexperimentales, teóricos y computacionales mediante el  programa  Xtrac.  Esta  simulación  considera deformaciones  y  comportamientos  en  diferentes estados  progresivos  de  carga  y  determina modelos gráficos de daño y plasticidad del material de concreto y acero.

  20. High field electron linacs

    High field electron linacs are considered as potential candidates to provide very high energies beyond LEP. Since almost twenty years not much improvement has been made on linac technologies as they have been mostly kept at low and medium energies to be used as injectors for storage rings. Today, both their efficiency and their performances are being reconsidered, and for instance the pulse compression sheme developed at SLAC and introduced to upgrade the energy of that linac is a first step towards a new generation of linear accelerators. However this is not enough in terms of power consumption and more development is needed to improve both the efficiency of accelerating structures and the performances of RF power sources

  1. Intense positron beams: linacs

    Beams of monoenergetic positrons with energies of a few eV to many keV have been used in experiments in atomic physics, solid-state physics and materials science. The production of positron beams from a new source, an electron linac, is described. Intense, pulsed beams of low-energy positrons were produced by a high-energy beam from an electron linac. The production efficiency, moderator geometry, beam spot size and other positron beam parameters were determined for electrons with energies from 60 to 120 MeV. Low-energy positron beams produced with a high-energy electron linac can be of much higher intensity than those beams currently derived from radioactive sources. These higher intensity beams will make possible positron experiments previously infeasible. 10 references, 1 figure

  2. Algoritmo del elipsoide interior para programación lineal

    Salamanca Fernández, Ángel; Juan Ruiz, Jesús

    1991-01-01

    En este artículo se desarrolla un algoritmo de puntos interiores para programación lineal a partir de consideraciones geométricas. En cada iteración del método se dispone de un punto interior al politopo. Con centro en dicho punto se obtiene un elipsoide interior a dicho politopo. La optimización de la función objetivo lineal sobre el elipsoide se obtiene mediante la solución de un problema de mínimos cuadrados. El punto resultante se adopta para la siguiente iteración. Se proponen dos método...

  3. Generalización en el estudio de funciones lineales

    Flores, Ángel; Chávez, Guadalupe

    2013-01-01

    En este artículo se presentan los avances de una investigación educativa que busca indagar los procesos de generalización de patrones en estudiantes de bachillerato en el Colegio de Ciencias y Humanidades de la UNAM (edades entre 15 y 17 años) y el papel que tales procesos juegan en el estudio de funciones lineales. Se buscó respuesta a la pregunta: ¿Cuál es el grado de entendimiento del concepto de función lineal en estudiantes de primer semestre de Bachillerato cuando su estudio parte de ac...

  4. Códigos binarios no lineales en MAGMA

    Ovalle Arce, Víctor

    2008-01-01

    La finalitat d'aquest projecte és aconseguir representar codis binaris no lineals de manera eficient en un ordinador. Per fer-ho, hem desenvolupat funcions per representar un codi binari a partir del super dual. Hem millorat la funció de càlcul del kernel d'un codi binari, implementada en projectes d'anys anteriors. També hem desenvolupat un paquet software per l'intèrpret MAGMA. Aquest paquet ens proveeix d'eines per al tractament de codis binaris no necessàriament lineals. La finalidad d...

  5. Sistema Inteligente para el álgebra lineal

    Casas, Laura; Pérez, Olga; Docampo, Lisandra; Mota, Yailé; Coello, Lenniet; González, Isabel; Martín, Ángela

    2013-01-01

    El trabajo describe la concepción del Sistema Inteligente para el Algebra Lineal (SIAL), el cual fue creado por los autores de la investigación. Sus fundamentos teóricos están relacionados con las técnicas de Inteligencia Artificial para clasificar, utilizando el clasificador k-vecinos más cercanos K-NN (Caballero, 2010), así como los cinco problemas tipos del Álgebra Lineal (Yordi, 2004). El SIAL se creó con el objetivo de apoyar al estudiante durante su estudio independiente para brindarle ...

  6. The Fermilab Linac Upgrade

    The Fermilab Linac Upgrade is planned to increase the energy of the H- linac from 200 to 400 MeV. This is intended to reduce the incoherent space-charge tuneshift at injection into the 8 GeV Booster which can limit either the brightness or the total intensity of the beam. The Linac Upgrade will be achieved by replacing the last four 201.25 MHz drift-tube tanks which accelerate the beam from 116 to 200 MeV, with seven 805 MHz side-coupled cavity modules operating at an average axial field of abut 7.5 MV/m. This will allow acceleration to 400 MeV in the existing Linac enclosure. Each accelerator module will be driven with a klystron-based rf power supply. A prototype rf modulator has been built and tested at Fermilab, and a prototype 12 MW klystron is being fabricated by Litton Electron Devices. Fabrication of production accelerator modules is in progress. 8 figs., 4 tabs

  7. The Fermilab Linac Upgrade

    Noble, R.J.

    1991-02-01

    The Fermilab Linac Upgrade is planned to increase the energy of the H- linac from 200 to 400 MeV. This is intended to reduce the incoherent space-charge tuneshift at injection into the 8 GeV Booster which can limit either the brightness or the total intensity of the beam. The Linac Upgrade will be achieved by replacing the last four 201.25 MHz drift-tube tanks which accelerate the beam from 116 to 200 MeV, with seven 805 MHz side-coupled cavity modules operating at an average axial field of abut 7.5 MV/m. This will allow acceleration to 400 MeV in the existing Linac enclosure. Each accelerator module will be driven with a klystron-based rf power supply. A prototype rf modulator has been built and tested at Fermilab, and a prototype 12 MW klystron is being fabricated by Litton Electron Devices. Fabrication of production accelerator modules is in progress. 8 figs., 4 tabs.

  8. TOP LINAC design

    The report describes a linear accelerator for protons named TOP LINAC designed for the TOP (Terapia Oncologica con Protoni, Oncological Protontherapy) project launched by the Italian National Institute of Health (Istituto Superiore di Sanita', ISS) to explore in collaboration with the biggest Oncological Hospital in Rome (Istituto Regina Elena, IRE) the potentialities of the therapy with accelerated protons and establish guide lines for the application of this new type of radiotherapy in comparison with the more traditional electron and x-rays radiotherapy. The concept of a compact accelerator for protontherapy applications bore within the Italian Hadrontherapy Collaboration (TERA Collaboration) with the aim to diffuse the protontherapy on the National territory. The ISS program plans to use the TOP linac proton beam also for production of PET (Positron Emission Tomography) radioisotopes and radiobiology studies. Official agreements are in course between ISS and ENEA which provides its experience in the industrial and medical accelerators for the design and the construction of the TOP linac. The accelerator that will be the first 3 GHz proton linac in the world, will be composed of a 428.3 MHz 7 Me V RFQ + DTL injector followed by a 7-65 Me V section of a 3 GHz SCDTL structure and a 65 - 200 Me V variable energy SCL 3 GHz structure. In particular the SCDTL section uses a highly innovative accelerating structure patented by ENEA. In this report the clinical and physical requests are discussed and a preliminary design of the whole machine is given

  9. Designing self-matching linacs

    The present trend in ion-linac design is to begin with a radio-frequency quadrupole (RFQ) linac followed by one or more drift-tube linac (DTL) tanks in which permanent-magnet quadrupoles are used for transverse focusing. The lack of adjustable elements (knobs) strongly suggests that one should seek linac designs with intertank matching solutions that are insensitive to beam currents and emittances, which can be accomplished if there are no sharp discontinuities in the focusing properties along the entire linac. Guidelines are presented for linac design and describe techniques for longitudinal as well as transverse matching between tanks. For a wide range of beam currents and emittances, a beam matched at the entrance to the RFQ should remain well matched throughout the entire linac

  10. Drift tubes of Linac 2

    1977-01-01

    With the advent of the 800 MeV PS Booster in 1972, the original injector of the PS, a 50 MeV Alvarez-type proton linac, had reached its limits, in terms of intensity and stability. In 1973 one therefore decided to build a new linac (Linac 2), also with a drift-tube Alvarez structure and an energy of 50 MeV. It had a new Cockcroft-Walton preinjector with 750 keV, instead of the previous one with 500 keV. Linac 2 was put into service in 1980. The old Linac 1 was then used for the study of, and later operation with, various types of ions. This picture shows Linac 2 drift-tubes, suspended on stems coming from the top, in contrast to Linac 1, where the drift-tubes stood on stems coming from the bottom.

  11. 43 CFR 10.14 - Lineal descent and cultural affiliation.

    2010-10-01

    ... 43 Public Lands: Interior 1 2010-10-01 2010-10-01 false Lineal descent and cultural affiliation..., folklore, oral tradition, historical, or other relevant information or expert opinion. (f) Standard of...) Document distinct patterns of material culture manufacture and distribution methods for the earlier...

  12. Estabilización robusta de sistemas lineales

    Horacio Leyva Castellanos

    2013-12-01

    Full Text Available En este trabajo se muestra un conjunto de resultados que permiten abordar el problema de la estabilización robusta de una familia de sistemas lineales positivos. Se describen dos nuevas aplicaciones en la teoría de control positivo para sistemas compartimentales y se muestra la aplicación de un teorema de robustez para tales sistemas

  13. Beam Loss in Linacs

    Plum, M A

    2016-01-01

    Beam loss is a critical issue in high-intensity accelerators, and much effort is expended during both the design and operation phases to minimize the loss and to keep it to manageable levels. As new accelerators become ever more powerful, beam loss becomes even more critical. Linacs for H- ion beams, such as the one at the Oak Ridge Spallation Neutron Source, have many more loss mechanisms compared to H+ (proton) linacs, such as the one being designed for the European Spallation Neutron Source. Interesting H- beam loss mechanisms include residual gas stripping, H+ capture and acceleration, field stripping, black-body radiation and the recently discovered intra-beam stripping mechanism. Beam halo formation, and ion source or RF turn on/off transients, are examples of beam loss mechanisms that are common for both H+ and H- accelerators. Machine protection systems play an important role in limiting the beam loss.

  14. Propiedades de las soluciones de sistemas estacionarios de la dinámica de poblaciones con difusión lineal y no lineal

    Suárez Fernández, Antonio

    1999-01-01

    En esta Memoria se estudian algunas de las propiedades de las soluciones de ciertas Ecuaciones en Derivadas Parciales no Lineales que modelan el comportamiento de dos especies que habitan en un mismo dominio y cuya difusión es, o bien, no lineal o lineal. En esta Memoria se estudian algunas de las propiedades de las soluciones de ciertas Ecuaciones en Derivadas Parciales no Lineales que modelan el comportamiento de dos especies que habitan en un mismo dominio y cuya difusión es, o bien, no...

  15. Injector linac of SPring-8

    The linac that is SPring-8 injector was completed and started operation from August 1. A beam was able to be transported to the final beam dumping at a tail end on August 8. From now on this linac carries out beam adjustment and be scheduled to do a beam injection to a synchrotron in October. The construction and fundamental performance of the linac are described. (author)

  16. Análisis contrastivo de la localización al español y catalán de los aceleradores en LibreOffice : estudio de los menús de la interfaz de usuario

    Ginovart Cid, Clara

    2015-01-01

    Esta tesina analiza la localización al español y catalán de los aceleradores de los menús de LibreOffice a través de la compilación de un corpus multilingüe que recoge las opciones de su interfaz de usuario. Al explotar el corpus, se observa que la tendencia en localización de aceleradores es no alejarse del original. Consideramos que la directriz de ser fiel al carácter o ubicación originales no satisface las necesidades de los usuarios, puesto que provoca aceleradores con trazos bajos y rep...

  17. NPL superconducting Linac control system

    The control system for the NPL Linac is based on a Microvax II host computer connected in a star network with 9 satellite computers. These satellites use single board varsions of DEC's PDP 11 processor. The operator's console uses high performance graphics and touch screen technology to display the current linac status and as the means for interactively controlling the operation of the accelerator

  18. Recent developments of the 1 MV AMS facility at the Centro Nacional de Aceleradores

    Scognamiglio, G.; Chamizo, E.; López-Gutiérrez, J. M.; Müller, A. M.; Padilla, S.; Santos, F. J.; López-Lora, M.; Vivo-Vilches, C.; García-León, M.

    2016-05-01

    The Centro Nacional de Aceleradores (CNA) hosts a 1 MV accelerator mass spectrometry (AMS) apparatus since September 2005. In order to improve its overall performance, several updates have been made on the existing facility during the last 10 years of operation. In this paper, two modifications conducted in 2015 will be described. To increase the transmission of the ions through the accelerator, the stripping gas on the 1 MV CNA machine was changed from Ar to He. The measured maximum transmission for almost every isotope results to be higher, especially for heavy masses: for instance, in the case of uranium in the 3+ charge state, the transmission increased from 11% with Ar gas to about 38% with He gas. The second advance consisted of the substitution of the existing gas ionization chamber with a new one provided by ETH Zurich. The ETH detector features with its miniaturized design and is optimized for low energy AMS (i.e. very low electronic noise and efficient charge collection). As the electronic noise is the most important contribution to the resolution for light ions, the total energy resolution has been reduced by 15% in the case of 10Be, allowing a better discrimination against its isobar, 10B. For the heaviest radionuclides where the quality of the spectra is determined by the charge carrier production in the gas, the resolution for 2.7 MeV uranium ions was improved by 30%, probably due to a more efficient charge collection.

  19. Accelerator-based research activities at 'Centro Nacional de Aceleradores', Seville (Spain)

    Respaldiza, M.A. [Centro Nacional de Aceleradores, Avd. Thomas A. Edison 7, E-41092 Sevilla (Spain); Departmento de Fisica Atomica, Molecular y Nuclear, Universidad de Sevilla, Sevilla (Spain)], E-mail: respaldiza@us.es; Ager, F.J. [Centro Nacional de Aceleradores, Avd. Thomas A. Edison 7, E-41092 Sevilla (Spain); Departmento de Fisica Aplicada I, Universidad de Sevilla, Sevilla (Spain); Carmona, A. [Centro Nacional de Aceleradores, Avd. Thomas A. Edison 7, E-41092 Sevilla (Spain); Laboratoire de Chimie Nucleaire Analytique et Bioenvironnementale, Universite de Bordeaux (France); Ferrer, J. [Centro Nacional de Aceleradores, Avd. Thomas A. Edison 7, E-41092 Sevilla (Spain); Garcia-Leon, M.; Garcia-Lopez, J. [Centro Nacional de Aceleradores, Avd. Thomas A. Edison 7, E-41092 Sevilla (Spain); Departmento de Fisica Atomica, Molecular y Nuclear, Universidad de Sevilla, Sevilla (Spain); Garcia-Orellana, I. [Centro Nacional de Aceleradores, Avd. Thomas A. Edison 7, E-41092 Sevilla (Spain); Gomez-Tubio, B. [Centro Nacional de Aceleradores, Avd. Thomas A. Edison 7, E-41092 Sevilla (Spain); Departmento de Fisica Aplicada III, Universidad de Sevilla, Sevilla (Spain); Morilla, Y. [Centro Nacional de Aceleradores, Avd. Thomas A. Edison 7, E-41092 Sevilla (Spain); Ontalba, M.A. [Centro Nacional de Aceleradores, Avd. Thomas A. Edison 7, E-41092 Sevilla (Spain); Departmento de Fisica, Universidad de Extremadura, Caceres (Spain); Ortega-Feliu, I. [Centro Nacional de Aceleradores, Avd. Thomas A. Edison 7, E-41092 Sevilla (Spain); Departmento de Fisica Atomica, Molecular y Nuclear, Universidad de Sevilla, Sevilla (Spain)

    2008-05-15

    In February 1998, almost 10 years ago, the set-up of the first IBA (ion beam analysis) facility in Spain took place with the arrival of a 3 MV tandem accelerator [J. Garcia-Lopez, F.J. Ager, M. Barbadillo-Rank, F.J. Madrigal, M.A. Ontalba, M.A. Respaldiza, M.D. Ynsa, Nucl. Instr. and Meth. B 161-163 (2000) 1137]. Since then, an intensive research program using IBA techniques has been carried out. Subsequently, a cyclotron for 18 MeV protons has been also installed at the 'Centro Nacional de Aceleradores' (CNA), devoted mainly to isotope production for PET (positron emission tomography) techniques, but possibly applied to material analysis and damage studies on a dedicated beam line. Moreover, a 1 MV tandem has been recently installed for AMS (accelerator mass spectrometry) {sup 14}C dating and environmental research with other isotopes. In the present paper we describe the new facilities and the developments of the 3 MV tandem beam lines occurred during the past years, as well as some examples of the most recent research activities in our Center in the fields of Material Science, Archaeometry, Biomedicine and Environment.

  20. Accelerator-based research activities at 'Centro Nacional de Aceleradores', Seville (Spain)

    In February 1998, almost 10 years ago, the set-up of the first IBA (ion beam analysis) facility in Spain took place with the arrival of a 3 MV tandem accelerator [J. Garcia-Lopez, F.J. Ager, M. Barbadillo-Rank, F.J. Madrigal, M.A. Ontalba, M.A. Respaldiza, M.D. Ynsa, Nucl. Instr. and Meth. B 161-163 (2000) 1137]. Since then, an intensive research program using IBA techniques has been carried out. Subsequently, a cyclotron for 18 MeV protons has been also installed at the 'Centro Nacional de Aceleradores' (CNA), devoted mainly to isotope production for PET (positron emission tomography) techniques, but possibly applied to material analysis and damage studies on a dedicated beam line. Moreover, a 1 MV tandem has been recently installed for AMS (accelerator mass spectrometry) 14C dating and environmental research with other isotopes. In the present paper we describe the new facilities and the developments of the 3 MV tandem beam lines occurred during the past years, as well as some examples of the most recent research activities in our Center in the fields of Material Science, Archaeometry, Biomedicine and Environment

  1. Plutonium measurements on the 1 MV AMS system at the Centro Nacional de Aceleradores (CNA)

    Plutonium isotopes have been recently added to the list of radionuclides that can be measured with the new generation of compact AMS facilities. In this paper we present first experimental results concerning the development of the plutonium AMS technique at 680 kV on the 1 MV AMS system at the Centro Nacional de Aceleradores (CNA) in Sevilla, Spain. This is the first compact AMS machine designed and manufactured by High Voltage Engineering Europa. As we demonstrate, the obtained backgrounds for 239,240Pu, of about 106 atoms, and the 239Pu/238U mass suppression factor, in the range of 10-9, compare to the ones achieved on other AMS facilities. With the measurement of reference materials provided by the International Atomic Energy Agency (IAEA-375, IAEA-Soil-6, IAEA-381) and samples already studied on the 600 kV compact ETH/PSI AMS system at Zuerich, we show that the CNA system can be perfectly used for the routine measurement of plutonium isotopes at environmental levels.

  2. Status of the compact 1 MV AMS facility at the Centro Nacional de Aceleradores (Spain)

    Since February 2006, the new 1 MV multielement compact AMS facility SARA (Spanish Accelerator for Radionuclides Analyses) at the Centro Nacional de Aceleradores (CNA) in Sevilla (Spain) is fully operative. During the first one and a half year of operation, the viability of the system for the measurement of 10Be, 14C, 129I and plutonium isotopes, 239Pu and 240Pu, has been evaluated. First results have demonstrated that, in terms of precision and detection limits, the performance of the device compares to other compact AMS facilities, although some progress can still be done in order to optimize its capacities. At this moment, background levels are in the order of 10-14 for 10Be/9Be, 10-13 for 129I/127I, 10-15 for 14C/12C (processed and unprocessed blank) and about 106 atoms for plutonium isotopes: 239Pu, 240Pu and 242Pu. In this work, the current status of the AMS measurements at CNA for the above mentioned radionuclides is described

  3. Radiological safety around a Linac of 18 MV; Seguridad radiologica alrededor de un LINAC de 18 MV

    Ceron R, P.; Rivera M, T. [IPN, Centro de Investigacion en Ciencia Aplicada y Tecnologia Avanzada, Calz. Legaria No. 694, Col. Irrigacion, 11500 Mexico D. F. (Mexico); Paredes G, L. [ININ, Carretera Mexico-Toluca s/n, 52750 Ocoyoacac, Estado de Mexico (Mexico); Azorin N, J. [Universidad Autonoma Metropolitana, Unidad Iztapalapa, San Rafael Atlixco No. 186, Col. Vicentina, 09340 Mexico D. F. (Mexico); Sanchez, A. [IPN, Escuela Superior de Fisica y Matematicas, Av. IPN s/n, Edif. 9, Col. San Pedro Zacatenco, 07738 Mexico D. F. (Mexico); Vega C, H. R., E-mail: victceronr@hotmail.com [Universidad Autonoma de Zacatecas, Unidad Academica de Estudios Nucleares, Cipres No. 10, Fracc. La Penuela, 09868 Zacatecas (Mexico)

    2014-10-15

    There are now several neutron detection systems, such as proportional counters based on BF{sub 3}, He{sub 3} and Bonner sphere spectrometers. However, the cost and complexity of the implementation of such systems makes them inaccessible for dosimetry purposes in radiotherapy rooms (Rt) and other facilities with this type of radiation fields. For these reasons the use of a neutron detection system is proposed composed by a paraffin moderator media forming an array 4π (spheres) and several pairs of thermoluminescent dosimeters TLD 600/TLD 700 inside, in order to make useful measurements for radiation protection around high-energy lineal accelerators (Linacs). In the first part of this work the system response when irradiated with a source of Pu Be and their corresponding calibration factor is displayed. In the second part are presented the ambient dose equivalent (H(10)) due to neutrons at various points of a living of Rt with a Linac of 18 MV, which are in the order mSv/Gy by X-ray treatment. The measurements made are similar to those taken in the memories of the accelerator and in previous work for this type of facility. (Author)

  4. Fuente de Alimentación para los Imanes Superconductores del Acelerador de Partículas Europeo XFEL

    García, O.; Francés, A.; J.M. Fernández; Varela, Pablo; Catalanotto, Giuseppe; Alou Cervera, Pedro; Oliver Ramírez, Jesús Angel; Asensi Orosa, Rafael; Prieto López, Roberto; Uceda Antolín, Javier; Cobos Márquez, José Antonio

    2013-01-01

    En este artículo se presenta la fuente de alimentación que se está diseñando para alimentar los imanes superconductores del acelerador de partículas europeo XFEL que se está construyendo en Hamburgo, cuyas características le hacen el más avanzado del mundo. Un imán superconductor es una carga muy inductiva que debe ser controlada en corriente y que presenta una caída de tensión muy baja cuando está en modo superconductor. La fuente debe ser capaz de alimentar esta carga con una alta fiabilida...

  5. Optimization of SRF Linacs

    Powers, Tom [JLAB

    2013-09-01

    This work describes preliminary results of a new software tool that allows one to vary parameters and understand the effects on the optimized costs of construction plus 10 year operations of an SRF linac, the associated cryogenic facility, and controls, where operations includes the cost of the electrical utilities but not the labor or other costs. It derives from collaborative work done with staff from Accelerator Science and Technology Centre, Daresbury, UK several years ago while they were in the process of developing a conceptual design for the New Light Source project.[1] The initial goal was to convert a spread sheet format to a graphical interface to allow the ability to sweep different parameter sets. The tools also allow one to compare the cost of the different facets of the machine design and operations so as to better understand the tradeoffs. The work was first published in an ICFA Beam Dynamics News Letter.[2] More recent additions to the software include the ability to save and restore input parameters as well as to adjust the Qo versus E parameters in order to explore the potential costs savings associated with doing so. Additionally, program changes now allow one to model the costs associated with a linac that makes use of energy recovery mode of operation.

  6. LINAC control automation system

    A 7 MeV Electron Beam Linear Accelerator (LINAC) being used for pulse radiolysis experiments at RC and CDD, B.A.R.C. has been automated with a PLC based control panel designed and developed by Computer Division, B.A.R.C.. The control panel after power on switches ON various units in a pre-defined sequence and intervals on a single turn of START key from OFF to ON position. The control panel also generates various ramp signals in a pre-defined sequence and rate and steady values and feeds to the LINAC bringing it to the ready for experiment condition. Similarly on a single turn of STOP key from OFF to ON position, the panel ramps down the various signals in pre-defined manners and makes OFF the various units in predefined sequence and timing providing safety to the machine. The steady values for various signals are on line settable as and when required so. This automation system relieves the operator from fatigue of time consuming manual ramping up or down of various signals and running around in four rooms for switching ON or OFF the various units enhancing efficiency and safety. This also facilitates the user scientist to do start up and shutdown operation in the absence of skilled operators and thus adds flexibility for working up to extended timing. This unit has been working satisfactorily since August 2002. For extraordinary condition automation to manual or vice versa change over has been provided. (author)

  7. Linealización entrada/salida de sistemas no lineales afines utilizando un filtro

    Alberto Delgado

    2011-01-01

    La linealización Entrada/Salida (E/S), dentro del marco teórico del control geométrico, es una técnica madura para sistemas no lineales afines. Esta técnica cancela los términos no lineales de la planta, usando una retroalimentación de estado no lineal, y produce una dinámica E/S lineal para la planta. En este artículo se muestra que un filtro D(s) puede utilizarse para Iinealizar sistemas no lineales afines en lugar de aplicar una retroalimentación de estado no lineal que requiere conocer la...

  8. Enseñanza de ecuaciones lineales en contexto

    Lydia R. Galagovsky; Cittadini, Paula E.

    2008-01-01

    Recientes estudios comparativos internacionales de evaluación del desempeño matemático en estudiantes secundarios han puesto de relieve dificultades y falta de destrezas para reconocer, formular y abordar problemas matemáticos en contextos reales. En este trabajo presentamos una propuesta didáctica innovadora para la enseñanza del tema ecuaciones matemáticas lineales, enmarcada en el contexto de las leyes económicas de Oferta, Demanda, y de Punto de Equilibrio entre precios y beneficios. Los ...

  9. ABP lactancia materna - regresión lineal

    Augusta Osorio Gonzales

    2011-01-01

    El objetivo que persigue el ABP “Lactancia materna” es el de poner al alcance de los alumnos de un curso de Estadística general, las herramientas básicas que le permitan establecer y analizar una recta de regresión lineal entre dos variables cuantitativas. El escenario o problema sobre el que se baso el ABP en el curso fue el resaltar la importancia de la Lactancia Materna, tema no vinculado normalmente con la Estadística, pero familiar para los alumnos (especialmente las damas), por lo cual ...

  10. Adaptividad para problemas de elasticidad lineal en 3D

    Prada, Claudio; Saliba, Roberto; Vénere, Marcelo J.

    1997-01-01

    En este trabajo se presenta un método adaptivo para resolver problemas de elasticidad lineal tridimensional por el método de elementos finitos incluyendo varias experiencias, tanto en la implementación como en la utilización del mismo. La estrategia de densificación está basada en la generación de redes encajadas mediante la subdivisión de elementos tipo simplices. Para la selección de los elementos a dividir se utiliza un indicador elemental de error, equivalente al error en la norma de la e...

  11. El Bloque lineal. Del Movimiento Moderno a la Contemporaneidad.

    Jiménez Romero, María Fátima

    2015-01-01

    Este trabajo se basa en el estudio , análisis , comprensión e investigación del bloque lineal (linear block ). Como ha llegado a ser la tipología residencial ( residential typology) de referencia para el alojamiento colectivo ( collective housing) así como la influencia de esta tipología en el desarrollo de la morfología (morphology ) de la ciudad. Se centrará la atención en la evolución que ha sufrido a lo largo de la historia, sus principales características, que lo definen como...

  12. Drift tubes of Linac 2

    Photographic Service

    1977-01-01

    Being redied for installation, those at the right are for tank 1, those on the left for tank 2. Contrary to Linac 1, which had drift-tubes supported on stems, here the tubes are suspended, for better mechanical stability.

  13. SLAC Linac Preparations for FACET

    Erickson, R.; Bentson, L.; Kharakh, D.; Owens, A.; Schuh, P.; Seeman, J.; Sheppard, J.C.; Stanek, M.; Wittmer, W.; Yocky, G.; Wienands, U.; /SLAC

    2011-02-07

    The SLAC 3km linear electron accelerator has been cut at the two-thirds point to provide beams to two independent programs. The last third provides the electron beam for the Linac Coherent Light Source (LCLS), leaving the first two-thirds available for FACET, the new experimental facility for accelerator science and test beams. In this paper, we describe this separation and projects to prepare the linac for the FACET experimental program.

  14. NPL superconducting linac control system

    The control system for the Nuclear Physics Lab (NPL) linac is based on a Microvax II host computer connected in a star network with nine satellite computers. These satellites use single-board versions of DEC's PDP 11 processor. The operator's console uses high-performance graphics and touch-screen technology to display the current linac status and as the means for interactively controlling the operation of the accelerator

  15. Inner structure of Linac 2

    1977-01-01

    With the advent of the 800 MeV Booster in 1972, the original injector of the PS, a 50 MeV Alvarez-type proton linac, had reached its limits, in terms of intensity and stability. In 1973 one therefore decided to build a new linac (Linac 2), also with a drift-tube Alvarez structure and an energy of 50 MeV. It had a new Cockcroft-Walton preinjector with 750 keV, instead of the previous one with 500 keV. Linac 2 was put into service in 1980. The old Linac 1 was then used for the study of, and later operation with, various types of ions. This picture shows the inner structure of Linac 2, with drift-tubes hanging on stems under a rigid support structure, soon to be mounted inside tank 1 (750 keV to 10 MeV, the lowest-energy one of 3). Frank Malthouse is standing in the background.

  16. Testing begins on Linac4

    Katarina Anthony

    2012-01-01

    On 3 August 2012, the Linac4 radiofrequency quadrupole (RFQ) module was installed at the accelerator test-stand in Building 152. The site will be the module’s home for almost a year, as the linear accelerator enters the assembly and testing stage.   Final module assembly is carried out before installation in Building 152.  Over the next Long Shutdown (LS2), Linac4 will replace the current Linac2 linear accelerator as the first link in CERN’s accelerator chain. It will deliver particles at 160 MeV to the PS Booster, more than triple the energy currently delivered by Linac2. But before the accelerator team can pop the champagne, the various elements of Linac4 will be tested and re-tested in facilities across CERN. “The first Linac4 tests are currently underway, starting with the CERN-built RFQ,” says Carlo Rossi, a physicist in the RF Group of the Beams (BE) Department and the RFQ project coordinator. “It’s an extremely impre...

  17. Induction Linac Pulsers

    The pulsers used in most of the induction linacs evolved from the very large body of work that was done in the U.S. and Great Britain during the development of the pulsed magnetron for radar. The radar modulators started at ∼100 kW and reached >10 MW by 1945. A typical pulse length was 1 μs at a repetition rate of 1,000 pps. A very comprehensive account of the modulator development is Pulse Generators by Lebacqz and Glasoe, one of the Radiation Laboratory Series. There are many permutations of possible modulators, two of the choices being tube type and line type. In earlier notes I wrote that technically the vacuum tube pulser met all of our induction linac needs, in the sense that a number of tubes, in series and parallel if required, could produce our pulses, regulate their voltage, be useable in feed-forward correctors, and provide a low source impedance. At a lower speed, an FET array is similar, and we have obtained and tested a large array capable of >10 MW switching. A modulator with an electronically controlled output only needs a capacitor for energy storage and in a switched mode can transfer the energy from the capacitor to the load at high efficiency. Driving a full size Astron induction core and a simulated resistive 'beam load' we achieved >50% efficiency. These electronically controlled output pulses can produce the pulses we desire but are not used because of their high cost. The second choice, the line type pulser, visually comprises a closing switch and a distributed or a lumped element transmission line. The typical switch cannot open or stop conducting after the desired pulse has been produced, and consequently all of the initially stored energy is dissipated. This approximately halves the efficiency, and the original cost estimating program LIACEP used this factor of two, even though our circuits are usually worse, and even though our inveterate optimists often omit it. The 'missing' energy is that which is reflected back into the line from

  18. Análisis de influencia en el modelo lineal general sesgo condicionado

    Muñoz Pichardo, Juan Manuel

    1992-01-01

    "Se propone una base teórica para abordar el problema del análisis de influencia a través del concepto de sesgo condicionado, aplicándose al modelo lineal general. Así, los resultados que se obtienen pueden ser trasladados a los distintos modelos lineale

  19. Linac transport and acceleration

    The acceleration of intense bunches maintaining high brightness is limited both by single-particle effects, e.g., misalignments, injection errors, and rf-steering, and collective phenomena, where the effects of the longitudinal and transverse wakefield on particles within a single bunch are the most severe. The working group has considered both problems and potentials of linac acceleration from ∼50 MeV to 1 GeV for free electron laser (FEL) applications, as well as from a few Gev to 1 TeV for linear colliders. The outlook for free electron lasers is bright: no fundamental problems seem to arise in the acceleration of peak currents in excess of 100 A with small emittance and low momentum spread. The situation of linear colliders is more complex and more difficult. Two examples, one operating at 11.4 GHz, the other at 30 GHz, are used to illustrate some of the difficulties and the exceedingly tight tolerances required. Both examples are based on round beams, and thus neither benefit from the advantages of flat beams nor address the increased care required in transporting beams of very small emittance in one plane. The working group acknowledges, but did not explore, promising concepts for colliders based on RF superconductivity

  20. Study of lineal and non-lineal transmission of an optical fiber Sagnac interferometer as a bidirectional device

    The optical fiber Sagnac interferometer is a versatile system that has been investigated for a variety of applications such as optical switchers, filters, demultiplexers and passive mode-locked laser. In many cases, this arrangement is designed using a symmetrical coupler with two of their ports connected making a loop and generally the analysis have been focused in the transmission of the signal propagated in only one direction. Therefore in the present work a complementary study of the system considering the analysis for the lineal and non-lineal transmission as a bidirectional device has been performed. The experimental setup consists of different optical fiber lengths inside the cavity loop (between 100 and 500 m) with highly twisted singlemode fiber, a quarter wave retarder placed asymmetrically in one arm and a 50/50 coupler. The results have shown that for low optical powers, it is possible to adjust the system transmission in both propagation directions with the rotation of the retarder wave. On the other hand, in high optical power levels, this arrangement showed that the transmission increases slowly for the case when both the input and the output beams have the same polarization. This behavior can be used for pedestal suppression in a light pulse. Furthermore, for the case when the output signal polarization is orthogonal respect to the input one, the transmission changes quite fast. This effect can be used for applications such as the passive mode-locking.

  1. Study of lineal and non-lineal transmission of an optical fiber Sagnac interferometer as a bidirectional device

    Ramos-Beltran, J [Benemerita Universidad Autonoma de Puebla, Facultad de Ciencias de la Electronica (Mexico); Beltran-Perez, G; Castillo-Mixcoatl, J; Munoz-Aguirre, S [Benemerita Universidad Autonoma de Puebla, Facultad de Ciencias Fisco-Matematicas (Mexico); Zaca-Moran, P [Benemerita Universidad Autonoma de Puebla, Fisicoquimica de Materiales, ICUAP (Mexico); Felipe, C, E-mail: squall_rb@hotmail.com [Departamento de biociencias e ingenieria, CIIEMAD, Instituto Politecnico Nacional (Mexico)

    2011-01-01

    The optical fiber Sagnac interferometer is a versatile system that has been investigated for a variety of applications such as optical switchers, filters, demultiplexers and passive mode-locked laser. In many cases, this arrangement is designed using a symmetrical coupler with two of their ports connected making a loop and generally the analysis have been focused in the transmission of the signal propagated in only one direction. Therefore in the present work a complementary study of the system considering the analysis for the lineal and non-lineal transmission as a bidirectional device has been performed. The experimental setup consists of different optical fiber lengths inside the cavity loop (between 100 and 500 m) with highly twisted singlemode fiber, a quarter wave retarder placed asymmetrically in one arm and a 50/50 coupler. The results have shown that for low optical powers, it is possible to adjust the system transmission in both propagation directions with the rotation of the retarder wave. On the other hand, in high optical power levels, this arrangement showed that the transmission increases slowly for the case when both the input and the output beams have the same polarization. This behavior can be used for pedestal suppression in a light pulse. Furthermore, for the case when the output signal polarization is orthogonal respect to the input one, the transmission changes quite fast. This effect can be used for applications such as the passive mode-locking.

  2. IH linac development at INS

    A new tuning method of the gap voltage distribution has been developed for an interdigital H type linac. With an asymmetrically ridged IH resonator, the voltage distribution was significantly improved by introducing a pair of Wing Tuners. The quality factor and the shunt impedance of the resonant cavity remained practically unchanged by these inductive tuning elements. The Wing Tuners strongly affect on linac characteristics similarly to the local reduction of the resonator diameter. A prototype IH linac has been constructed to demonstrate the operational capabilities of the tuning method. The linac is designed to accelerate protons from an energy of 15 to 161 keV with an rf frequency of 100 MHz. The linac tank is made of mild steel, and 48 and 92 cm in diameter and in length, respectively. The drift tube structure of π/3π mode is adopted, and an electrostatic quadrupole lens is installed in every 3π drift tube. The experimental results of the proton model agree well with the design characteristics. (author)

  3. Explorando sistemas dinámicos 3d no lineales

    Haramburu, Pablo; Delrieux, Claudio

    2005-01-01

    La finalidad de la Visualización Científica es ayudar en la comprensión y el análisis de determinados problemas científicos. Un modelo matemático utilizado muy frecuentemente para la representación de problemas reales en muchas disciplinas es el de los sistemas dinámicos. Es posible encontrarlos en ecología, electrónica, mecánica no lineal, dinámica de fluídos, matemática, economía, etc. En la mayoría de los casos, estos sistemas no son resolubles en forma analítica, por lo que su adecuada...

  4. Simulacion borrosa de un reactor con reaccion exotermica no lineal

    MIGUEL ANGEL RODRIGUEZ BORROTO

    2007-01-01

    Full Text Available En el presente trabajo se desarrolla un modelo difuso basado en la estructura Takagi-Sugeno-Kang dinámica para un reactor continuo de tanque con agitador (RCTA con reacción química de primer orden exotérmico. A partir de datos experimentales obtenidos mediante simulación del proceso real, se obtiene la base de datos de las variables de entrada y salida del proceso y a partir de la misma se elaboran los archivos de datos de entrenamiento y de verificación del modelo borroso el cual es obtenido mediante la herramienta anfis de MATLAB. El modelo obtenido permite predecir la salida del sistema con errores de predicción muy bajos, por lo que el mismo sienta las bases para el diseño de un controlador predictivo no lineal del mismo en próximas etapas de la investigación

  5. Status of the RFD Linac Structure Developement

    Swenson, Donald A.

    2000-01-01

    The Proof-of-Principle (POP) prototype of the Rf-Focused Drift tube (RFD) linac structure is currently under test at Linac Systems, after years of delay due to a variety of technical problems. A discussion of these technical problems and their solutions will be presented. The status of these tests will be reported. Plans for future development of this linac structure will be revealed. Potential uses of this linac structure for a variety of scientific, medical, and industrial applications will...

  6. Upgrading the Fermilab Linac local control system

    A new control system for the Fermilab Linac is being designed, built and implemented. First, the nine-year-old linac control system is being replaced. Second, a control system for the new 805 MHz part of the linac is being built. The two systems are essentially identical, so that when the installations are complete, we will still have a single Linac Control System. 8 refs., 5 figs

  7. Linac3 - 1992-1994

    CERN; A Van der Shueren; Jean-Claude Vialis

    1995-01-01

    This film reports the differents steps of the construction in differents places (Italy, Germany, France) from 29 October 1992 to 29 April 1994. This linac, commissioned in summer 1994, presently provides beams of 208Pb53+. A 14 GHz ECR ion source operating in the "afterglow" mode produces Pb 27+ ions at 2.5 keV/u. This beam is accelerated in an RFQ and a three tank IH linac to 4.2 MeV/u where stripping in a 1 um carbon foil to a charge state distribution centered around Pb53+ takes place. 53+ ions are selected from this mixture in a magnetic filter before being transported to the PS Booster and other circular machines. Linac3, the more common name for this machine, was built by a truly international collaboration involving France, Italy, Germany, Italy, Sweden, Switzerland, India, the Czech Republic and CERN.

  8. RF system of FELI linac

    FELI (Free Electron Laser Research Institute, Inc.) is constracting a Free Electron Laser facility covering from 20μm (infrared region) to 0.35μm (ultra violet region), using an S-band linac. The building will be completed in November 1993 and linac will start to be installed in December 1993. RF system of linac for FEL is required of long pulse duration and high stability. An S-band klystron (Toshiba E3729) is operated in three pulse operation modes (pulse width and peak RF power); 24μs-24MW, 12.5μs-34MW, 0.5μs-70MW. Each klystron modulator has the PFN consisting of 4 parallel networks of 24 capacitors and 24 inductors, and it has a line switch of optical thyristor stack. (author)

  9. Cálculo no lineal de estructuras reticuladas y laminares

    Ortiz Herrera, Jesús

    1976-02-01

    Full Text Available By many of electronic calculus it is possible to approach the non linear analysis of bar constructions efficiently and without the limitations of the traditional plastic Calculus. In order to prove this statement, the author presents certains structural analysis that have been carried out by means of techniques and calculation programs of his own. Further, the non linear analysis of revolving sheets is presented to which algorithms of great formal similarity to those in the case of bar constructions are applicable. Both for these latter ones as weil as for laminated structures the programs elaborated by the author allow a great variety of anelastic analyses (and as a special case, of elastic analysis.Con la ayuda del cálculo electrónico, el análisis no lineal de estructuras de barras es abordable con eficiencia y sin caer en las limitaciones del cálculo plástico tradicional. Con objeto de probar esta afirmación, se presentan determinados análisis estructurales realizados mediante técnicas y programas de cálculo propios. Se presenta asimismo el análisis no lineal de láminas de revolución, a las cuales son aplicables algoritmos de gran similitud formal con los del caso de estructuras de barras. Tanto para estas últimas como para las estructuras laminares, los programas desarrollados por el autor permiten efectuar gran variedad de análisis inelásticos (y elásticos como caso particular.

  10. IMPACT simulation and the SNS linac beam

    Multi-particle tracking simulations for the SNS linac beam dynamics studies are performed with the IMPACT code. Beam measurement results are compared with the computer simulations, including beam longitudinal halo and beam losses in the superconducting linac, transverse beam Courant-Snyder parameters and the longitudinal beam emittance in the linac. In most cases, the simulations show good agreement with the measured results

  11. Cockcroft-Walton generator for Linac 2

    Photographic Service

    1976-01-01

    Its higher voltage of 750 kV, compared to the 520 kV Cockcroft-Walton of Linac 1, contributed to the higher current that Linac 2 could deliver. The cubic container houses the electronics. The ion-source, in the spherical container, delivered protons and, for tests, also deuterons. In 1993 an RFQ replaced it as Linac 2 preinjector.

  12. SUPERCONDUCTING LINAC FOR THE SPALLATION NEUTRON SOURCE

    The Spallation Neutron Source (SNS) linac is comprised of both normal and superconducting rf (SRF) accelerating structures. The SRF linac accelerates the beam from 186 to 1250 MeV through 117 elliptical, multi-cell niobium cavities. This paper describes the SRF linac architecture, physics design considerations, cavity commissioning, and the expected beam dynamics performance

  13. Intrabeam stripping in H- Linacs

    Lebedev, V; Ostigy, J -F; Alexandrov, A; Shishlo, A

    2012-01-01

    A beam loss in the superconducting part of the SNS linac has been observed during its commissioning and operation. Although the loss does not prevent the SNS high power operation, it results in an almost uniform irradiation of linac components and increased radiation levels in the tunnel. Multi-particle tracking could neither account for the magnitude of the observed loss nor its dependence on machine parameters. It was recently found that the loss is consistent with the intrabeam particle collisions resulting in stripping of H- ions. The paper describes experimental observations and corresponding analytical estimates of the intrabeam stripping.

  14. Decisiones financieras con programación lineal: diferentes estados de la naturaleza

    Paulino E. Mallo; Artola, María Antonia; Morettini, Mariano

    2009-01-01

    Desde los inicios de la investigación operativa la programación lineal ha sido una de sus herramientas más eficientes y difundidas. En el campo financiero también se ha dado lugar a la aplicación de la programación lineal, aunque con menos frecuencia que en la faz productiva. Sin embargo, los supuestos de la programación lineal no siempre se satisfacen acabadamente en la realidad. Algunas de las situaciones enfrentadas son de certeza, satisfaciendo los supuestos que requiere la técnica, pero ...

  15. Modelo no lineal con potencial Seno-Gordon para un cristal fotónico unidimensional

    Margarita Franco Ortíz; Adalberto Corella Madueño; Juan Adrián Reyes Cervantes; Arnulfo Castellanos Moreno; Rodrigo Arturo Rosas Burgos

    2013-01-01

    Se presenta un modelo para un cristal fotónico unidimensional formado por una sucesión de planos constituidos por material no lineal, inmersos en un medio lineal. Se resuelve la ecuación de Schrödinger introduciendo en el hamiltoniano modelo del cristal un potencial no lineal tipo Seno-Gordon. Se obtiene analíticamente una versión generalizada, dependiente de la amplitud de la onda incidente, de la ecuación trascendente que caracteriza al modelo del cristal de Kronig-Penney, de donde se dete...

  16. Drift Tube Linac Conditioning of Tank1

    Shafqat, N; Toor, W A

    2014-01-01

    Tank1 of the Drift Tube Linac (DTL) of the Linac4 has been conditioned at the Linac4 tunnel. The tank was tuned for resonance at 352.2 MHz, and stable operation has been achieved with 725 µs long RF pulses at a repetition rate of 1 Hz. The maximum RF level that has been reached is 810 kW with a pulse width of 600 µs. Since this was the first RF structure exclusively conditioned in the Linac4 tunnel with the operation and control software of Linac4, some related issues and limitations had to be taken into account.

  17. Emittance growth in rf linacs

    As the space-charge limit is approached, the current that can be accelerated in an rf linac and the output emittance that can be expected are discussed. The role of the envelope equations to estimate limits is outlined. The results of numerical experiments to explore general properties of emittance growth are given

  18. Design of long induction linacs

    A self-consistent design strategy for induction linacs is presented which addresses the issues of brightness preservation against space charge induced emittance growth, minimization of the beam breakup instability and the suppression of beam centroid motion due to chromatic effects (corkscrew) and misaligned focusing elements. A simple steering algorithm is described that widens the effective energy bandwidth of the transport system

  19. The new Linac moves mountains

    2008-01-01

    The civil engineering work has started for Linac 4, one of the major renovation projects for the CERN accelerator complex. The work will be completed at the end of 2010 and the new linear accelerator is scheduled to be commissioned in 2013.

  20. Prototype of the RFD linac structure

    A 2.5-MeV prototype of a 'Compact 12-MeV Proton Linac for PET Isotope Production' is under construction at Linac Systems. This unit will serve as the 'proof of principle' for the revolutionary new Rf Focused Drift tube (RFD) linac structure. Both the prototype and the production unit will operate at 600 MHz. The prototype comprises a 25- keV proton ion source, a short LEBT, a 0.65-m-long RFQ linac to 0.8 MeV, and a 0.35-m-long RFD linac to 2.5 MeV. Because of the similarity of the accelerating and focusing properties of the RFQ and RFD linac structures, no matching section is required between them. The two linac structures will be resonantly coupled together and powered by a collection of planar triodes. The prototype is scheduled for completion in the fall of 1997. (author)

  1. Progress in design of the SNS linac

    The Spallation Neutron Source (SNS) is a six-laboratory collaboration to build an intense pulsed neutron facility at Oak Ridge, TN. The linac design has evolved from the conceptual design presented in 1997 in order to achieve higher initial performance and to incorporate desirable upgrade features. The linac is now designed to produce 2-MW beam power using a combination of radio-frequency quadrupole (RFQ) linac, drift-tube linac (DTL), coupled-cavity linac (CCL), and superconducting-RF (SRF) linac. Designs of each of these elements support he high peak intensity and high quality beam required for injection into the SNS accumulator ring. This paper will trace the evolution of the linac design and the progress made in the R and D program. (author)

  2. PROGRESS IN DESIGN OF THE SNS LINAC

    R. HARDEKOPF

    2000-11-01

    The Spallation Neutron Source (SNS) is a six-laboratory collaboration to build an intense pulsed neutron facility at Oak Ridge, TN. The linac design has evolved from the conceptual design presented in 1997 to achieve higher initial performance and to incorporate desirable upgrade features. The linac will initially produce 2-MW beam power using a combination of radio-frequency quadruple (RFQ) linac, drift-tube linac (DTL), coupled-cavity linac (CCL), and superconducting-cavity linac (SCL). Designs of each of these elements support the high peak intensity and high quality beam required for injection into the SNS accumulator ring. This paper will trace the evolution of the linac design, the cost and performance factors that drove architecture decisions, and the progress made in the R&D program.

  3. Progress in design of the SNS linac

    Hardekopf, R. [Los Alamos National Laboratory, Los Alamos, NM (United States)

    2001-03-01

    The Spallation Neutron Source (SNS) is a six-laboratory collaboration to build an intense pulsed neutron facility at Oak Ridge, TN. The linac design has evolved from the conceptual design presented in 1997 in order to achieve higher initial performance and to incorporate desirable upgrade features. The linac is now designed to produce 2-MW beam power using a combination of radio-frequency quadrupole (RFQ) linac, drift-tube linac (DTL), coupled-cavity linac (CCL), and superconducting-RF (SRF) linac. Designs of each of these elements support the high peak intensity and high quality beam required for injection into the SNS accumulator ring. This paper will trace the evolution of the linac design and the progress made in the R and D program. (author)

  4. Florida State University superconducting linac

    As early as the fall of 1977 it was decided that the future research needs of their nuclear structure laboratory required an increase in energy capability to at least 8 MeV per nucleon for the lighter ions, and that these needs could be met by the installation of a 17 MV tandem Van de Graaff accelerator. The chief problem with this proposal was the high cost. It became apparent that a far less expensive option was to construct a linear accelerator to boost the energy from their existing 9 MV tandem. The options open to them among linac boosters were well represented by the room temperature linac at Heidelberg and the superconducting Stony Brook and Argonne systems. By the Spring of 1979 it had been decided that both capital cost and electric power requirements favored a superconducting system. As regards the two superconducting resonator technologies - the Argonne niobium-copper or the Caltech-Stony Brook lead plated copper - the Argonne resonators, though more expensive to construct, had the advantages of more boost per resonator, greater durability of the superconducting surface and less stringent beam bunching requirements. In 1980 pilot funding from the State of Florida enabled the construction of a building addition to house the linac and a new target area, and the setting up of a small, three resonator, test booster. Major funding by the NSF for the laboratory upgrade started in 1984. With these funds they purchased their present helium liquefaction and transfer system and constructed three large cryostats, each housing four Argonne beta = 0.105 resonators and two superconducting solenoids. The last large cryostat was completed and installed on-line early this year and the linac was dedicated on March 20. Nuclear physics experiments using the whole linac began in early June. 4 references, 6 figures, 1 table

  5. BNCT with linac, feasibility study

    High energy photon beams from Medical Linear Accelerators (linacs) which are used in radiotherapy produce undesirable neutrons, beside the clinically useful electron and photon beams. Neutrons are produced from the photonuclear reaction (γ,n) of high energy photons with high Z-materials which compose the accelerator head. In this paper the possible use of these undesirable neutrons for BNCT is investigated, making use of high energy linacs already installed in hospitals, primarily for high energy electron and photon therapy and applying them in the context of BNCT. The photoneutron components emitted by the accelerator is the source for Monte Carlo simulations of the interactions that take place within the head of a voxel-based phantom. The neutron flux across the phantom head is calculated using different moderator arrangements and different techniques in the aim of increasing the thermal neutron flux at the targeted site. Also, we shall test different configurations of the linac head to maximize the exposure of high-Z materials to the photon beam, including the removal of the flattening filter, so as to boost the photoneutron production in the linac head. Experimental work will be conducted in hospitals to validate the Monte Carlo simulations. To make use of linacs for BNCT will be advantageous in the sense that the setting in a hospital department is much more acceptable by the public than a reactor installation. This will mean less complications regarding patient positioning and movement with respect to the beams, additional patient transportation and management will be more cost effective. (author)

  6. first tank of Linac 1

    This was the first tank of the linear accelerator Linac1, the injection system for the Proton Synchrotron, It ran for 34 years (1958 - 1992). Protons entered at the far end and were accelerated between the copper drift tubes by an oscillating electromagnetic field. The field flipped 200 million times a second (200 MHz) so the protons spent 5 nanoseconds crossing a drift tube and a gap. Moving down the tank, the tubes and gaps had to get longer as the protons gained speed. The tank accelerated protons from 500 KeV to 10 MeV. Linac1 was also used to accelerate deutrons and alpha particles for the Intersecting Storage Rings and oxygen and sulpher ions for the Super Proton Synchrotron heavy ion programme.

  7. Análisis de pérdida de estabilidad no lineal de elementos estructurales sometidos a compresión. // Slender structural elements non lineal stability analysis.

    C. Fabré Sentile

    2007-01-01

    Full Text Available En el presente artículo se muestra el análisis de perdida de estabilidad en elementos estructurales delgados bajocompresión. Se realiza la exposición de las consideraciones del análisis lineal y no lineal de perdida de estabilidad y seejemplifica con una estructura modelada mediante elementos finitos, estableciéndose conclusiones interesantes.Palabras claves: Estructuras esbeltas, estabilidad no-lineal, Euler.______________________________________________________________________________Abstract:Presently paper deals with stability analysis in structural elements. The considerations of lineal and non lineal analysis ofstability are exposed and it is exemplified with a finite element structure model, settling down interesting conclusions.Key words: Slender structures, non-lineal stability, Euler.

  8. Harmonic Analysis of Linac Alignment

    McCrady, Rodney C

    2005-01-01

    We have analyzed the requirements on alignment of the focusing elements (quadrupole doublets) in the Los Alamos Neutron Science Center (LANSCE) side coupled linac. The analysis is performed in terms of harmonics of the quardrupole spacing. This allows us to determine the effect of intentional deviations from a straight line, such as following the curvature of the Earth, and of unintentional deviations introduced by measurement and alignment errors. Results are compared to measured positions of the doublets.

  9. Programación lineal aplicada al cálculo plástico elemental de estructuras lineales

    Antón Corrales, J. M.

    1970-06-01

    Full Text Available A method is described for elementary calculations of linear structures, under non elastic conditions, and subjected to point loads. The method involves the use of Simplex programs, which are already available for any scientific computer. The result gives either a factor of safety for a structure that has already been designed, or else an optimum design for given conditions. The calculation is very short for one loading system, and less so, if several loading conditions are assumed. The method can be further improved, thus rendering its use even more simple.Expone este artículo un método para hacer los cálculos plásticos elementales de estructuras lineales con cargas puntuales por medio de programas Simplex, ya disponibles en cualquier ordenador científico, dando como resultado, sea un coeficiente de seguridad de una estructura ya dimensionada, sea una optimización de la misma. El cálculo es muy corto con un caso de cargas, y menos con varios casos de cargas. El método admite perfeccionamientos, que pueden hacer todavía más elemental su introducción en computador.

  10. Linacs for medical and industrial applications

    Linear accelerators for medical and industrial applications have become an important commercial business. Microwave electron linacs for cancer radiation therapy and high-energy industrial radiography form the bulk of this market, but these, as well as induction linacs, are now being offered for radiation processing applications such as sterilization of disposable medical products, food preservation and material modifications. The radio frequency quadrupole (RFQ) linac has now made the ion linac also practical for commercial applications in medicine and industry, including radiation therapy, isotope production, neutron production, materials modification, and energy transfer processes. Ion linacs for several of these applications will soon be commercially available. The market for both ion and electron linacs is expected to significantly grow in several exciting and important areas

  11. Application of shielding calculation of high-energy linear accelerators based on the NCRP-151 protocol; Aplicacion de calculo de blindajes de aceleradores lineales de alta energia basada en el protocolo NCRP-151

    Torres Pozas, S.; Monja Rey, P. de la; Sanchez Carrasca, M.; Yanez Lopez, D.; Macias Verde, D.; Martin Oliva, R.

    2011-07-01

    In recent years, the progress experienced in cancer treatment with ionizing radiation can deliver higher doses to smaller volumes and better shaped, making it necessary to take into account new aspects in the calculation of structural barriers. Furthermore, given that forecasts suggest that in the near future will install a large number of accelerators, or existing ones modified, we believe a useful tool to estimate the thickness of the structural barriers of treatment rooms. The shielding calculation methods are based on standard DIN 6847-2 and the recommendations given by the NCRP 151. In our experience we found only estimates originated from the DIN. Therefore, we considered interesting to develop an application that incorporates the formulation suggested by the NCRP, together with previous work based on the rules DIN allow us to establish a comparison between the results of both methods. (Author)

  12. Use of a detector CZT for verification of shields against neutron in 3 linear accelerators in clinical use; Uso de un detector CZT para la verificacion de blindajes frente a neutrones en 3 aceleradores lineales de uso clinico

    Barquero Sanz, R.; Anton, D. A.; Iniguez de la Torre, P. L.; Castillo Belmonte, A. C. del; Alonso, D. A.; Miguel, D. M. de; Lopez Lara-Martin, F. L.

    2013-07-01

    This paper describes how to use the reaction of thermal neutrons (n?) {sup 1}13Cd, {sup 1}14 Cd with the cadmium in an alloy of cadmium and zinc Telluride (CZT) semiconductor detector. 558 keV photons produced can be detected by the own semiconductor. In this way have an agile method for the measurement of the neutron flux transmitted by shielding and which provides an almost immediate reading of the result. This method applies three accelerators linear in that checks the correct shield on their respective treatment rooms. (Author)

  13. Simulación y validación experimental de la dosimetría de campos pequeños de fotones en un acelerador lineal de electrones

    Fernández, María Luz

    2014-01-01

    La utilización de campos pequeños de fotones en radioterapia, se puede distinguir principalmente por dos efectos: la pérdida del equilibrio electrónico lateral y la oclusión de la fuente. Ambos resultan en una disminución del rendimiento del haz en el eje central y en una extensión de la zona de penumbras en los perfiles. Estos efectos son difíciles de cuantificar ya que los detectores de tamaño similar o mayor que el campo de radiación presentan imprecisiones en las medidas. Las técnicas num...

  14. Characterization with GEANT4 of 16OMLCTM Siemens multi leaf collimator in a linear accelerator Siemens OncortM; Caracterizacion con GEANT4 colimador multilaminas siemenes 160-MLC{sup T}M en un acelerador lineal Siemens Oncor

    Cortes Giraldo, M. A.; Miras, H.; Arrans, R.; Gallardo, M. I.; Quesada, J. M.

    2011-07-01

    The interest and motivation of this work lies in the ability to present GEANT4 to simulate neutron transport through the material, making it possible to make estimates of pollution existing neutron radiotherapy treatments to energies at which the neutron production is significant.

  15. Craniospinal treatment with IMRT multi-isocentric and image-guided linear accelerator based on Gantry; Tratamiento craneoespinal multi-isocentrico con IMRT y guiado por imagen en acelerador lineal basado en Gantry

    Sanz Beltran, M.; Caballero Perea, B.; Rodriguez Rodriguez, C.; Arminio Diaz, E.; Lopez Fernandez, A.; Gomez Fervienza, J. R.; Crespo Diez, P.; Cantarero Valenzuela, N.; Alvarez Sanchez, M.; Martin Martin, G.; Gomez Fervienza, J. r.; Crespo Diez, P.; Cantarero Valenzuela, N.; Alvarez Sanchez, M.; Martin Martin, G.

    2011-07-01

    The objective is the realization of craniospinal treatment with a linear accelerator equipped with gantry based on MLC, carbon fiber table and Image Guided capability. The great length of treatment (patient l, 80m in height) was a great difficulty for want of full length of the longitudinal movement of the table to adequately cover the PTV, plus free metallic screws fastening the head of the table extender preventing further incidents.

  16. Study of technical and economic feasibility of using a portal dosimetry system for quality control of linear accelerators; Estudio de viabilidad tecnica y economica del uso de un sistema de dosimetria portal para el control de calidad de aceleradores lineales

    Fax, X.; Piro, N.; Sanchez, N.; Toribio, I.; Hermida, M.; Seioane, A.; Saez, J.; Beltran, M.

    2011-07-01

    We have studied the feasibility of Varian portal vision system AS500-II, dosimetry calibration mode, as a substitute for radiochromic plates in quality control tests that required the use of such film. Over a period of two months have been analyzed both the dosimetric characteristics of the system and the mechanical positioning. In addition there has been a financial estimate of annual savings that would result from replacing the radiochromic film by the portal system in a multi-energy accelerator.

  17. Licensing process and implementation of a mobile linear accelerator for treatment of intraoperative radiation therapy; Proceso de licenciamiento e implantacion de un acelerador lineal movil para tratamientos de radioterapia intraoperatoria

    Sierra Diaz, F.; Gonzalez Ruiz, C.; Garcia Marcos, R.; Gallego Franco, P.; Rodriguez Checa, M.; Gomez Calvar, R.; Lopez Bote, M. A.

    2013-07-01

    The objective is to show how the working procedures, have been defined unambiguously to ensure together with the structure of the installation, and optimally located elements of radiation protection, compliance with the classification of areas, occupation factors and rates expected according to them. (Author)

  18. Modelling of linear accelerator table for use in the design of 3D and VMAT radiotherapy treatments; Modelizacion de mesa de acelerador lineal para aplicacion en los disenos de tratamientos radioterapicos 3D y VMAT

    Velazquez Miranda, S.; Jimenez Domingiuez, M.; Mateos Perez, J. C.; Herrador Cordoba, M.

    2011-07-01

    The new design of carbon treatment tables for rotational IMRT application is being submitted in multiple publications, all dosimetric test to determine their influence on treatment. In most publications can be concluded that their influence is not negligible, especially in near-horizontal angles. In the case of IMRT its influence becomes non-intuitive and therefore difficult to estimate. These publications can not consider all the possibilities of clinical practice, so that its applicability is limited. We propose, therefore, a role-table with the exact geometry of the treatment and density adjusted to the experimental data, to resolve the estimation of their influence in each clinical case.

  19. Quality control of virtual wedge in a linear electron accelerator with a computerized radiography system (CR); Control de calidad de la cuna virtual en un acelerador lineal de electrones mediante un sistema de radiografia competerizada (CR)

    Ordiales, J. M.; Alvarez, F. J.; Falero, B.

    2011-07-01

    For quality control of the virtual wedge there are several systems on the market as arrays of detectors or ionization chambers, linear or 2D configuration, radiochromic films or digital imaging systems incorporated in electron linear accelerators (ALE ). The present work aims at implementing a system of Computed Radiography (CR) for a routine check of the virtual wedge.

  20. Evaluation of a dispersion medium for the irradiation of blood products in a electron linear accelerator; Evaluacion de un medio dispersor para la irradiacion de hemoderivados en un acelerador lineal de electrones

    Ordiales, J. M.; Falero, B.; Vazquez, M.; Alvarez, F. J.

    2013-07-01

    The use of bags of rice as dispersion medium in irradiation of blood products for medical use is less effective than the immersion from the point of view dosimetric water. However, given the wide range of dose values for a valid result and once subjected to quality control procedure, the method provides the necessary work for the irradiation of blood products in a linear electron accelerator. (Author)

  1. Diagnostic expert system in the PF LINAC

    A prototype diagnostic expert system (ES) was developed for the Photon Factory 2.5-GeV electron/positron LINAC injector system. The ES has been on-lined with the conventional linac computer network for receiving real data. This project was undertaken in an attempt to reduce the linac operator's mental workload, diagnosis duties, and to explore Artificial Intelligence (AI) technologies. The outlook for ES and its problems, and what has been achieved are outlined in this presentation. (author)

  2. ABP lactancia materna - regresión lineal

    Augusta Osorio Gonzales

    2011-07-01

    Full Text Available El objetivo que persigue el ABP “Lactancia materna” es el de poner al alcance de los alumnos de un curso de Estadística general, las herramientas básicas que le permitan establecer y analizar una recta de regresión lineal entre dos variables cuantitativas. El escenario o problema sobre el que se baso el ABP en el curso fue el resaltar la importancia de la Lactancia Materna, tema no vinculado normalmente con la Estadística, pero familiar para los alumnos (especialmente las damas, por lo cual en la ejecución del ABP se incorporó la temática relacionada con la poca información e interés que muestran los varones en el tema. En el escenario, se creó una ONG ficticia llamada ALACTAR, la que estaba interesada en crear un tríptico de información dirigida a los varones, en el que se resalten los beneficios que proporciona la Lactancia Materna en el infante y la madre que da de lactar. Entre los temas a resaltar, se encuentran el incremento del Coeficiente Intelectual, la disminución de la Obesidad Infantil, la disminución de la Diabetes Juvenil y la disminución en el riesgo de la madre de contraer Cáncer de ovarios. La idea es utilizar datos de investigaciones que se han hecho en el país que tiene en su poder ALACTAR y que aún no se han procesado apropiadamente. Dentro de la metodología ABP, se usaron como herramientas las siguientes: foros, horas de trabajo en aula y la confección de un trabajo final que consiste en un tríptico o póster para ALACTAR.

  3. Dual mode medical Linac development at SAMEER

    SAMEER has developed a 6 MV Oncology machine. These types of machines are already tested and treating patients at Head and Neck Cancer Institute, Indore and Adyar Cancer Hospital at Chennai. Two more such machines are in the process of commissioning at Amravati Cancer Foundation, Amravati and B K L Walawalkar Hospital, Dervan. For treating malignant tumors, high energy X-rays are required and for treatment of skin cancer electrons are used. Therefore, to enhance the present low energy radiotherapy linac technology at SAMEER, a dual photon energy linac capable of giving 6 and 15 MV photons and multiple electron energies (6, 8, 10, 12, 14, 16 and 18 MeV) for treatment is being developed indigenously. The prototype of a 15 MeV linac is already developed and tested at SAMEER. The sub-assemblies for the dual mode medical linac like gridded electron gun and target is designed and tested. A linac tube with a detuning plunger or energy switch is designed and assembled. The linac is tuned and tested at low power. The measured parameters are given. Outgassing of linac tube was carried out at a temperature of 250 C. The vacuum achieved after baking is ∼10-10 mbar. The linac tube is now integrated on the gantry head for high power testing. This paper will discuss the design, experimental measurement results and vacuum processing aspects of the linac tube. (author)

  4. Linac-LHC EP Collider Options

    Zimmermann, F; Bordry, Frederick; Braun, H H; Brüning, Oliver Sim; Çiftçi, A K; Chattopadhyay, S; Dainton, J B; de Roeck, A; Eide, A; Garoby, R; Holzer, B J; Klein, M; Linnecar, T; Mess, K H; Osborne, J; Rinolfi, L; Schulte, D; Sultansoy, S; Tomás, R; Tückmantel, Joachim; Vivoli, A; Willeke, F J

    2008-01-01

    We describe various parameter scenarios for a ring-linac ep collider based on LHC and an independent electron linac. Luminosities between $10^{31}$ and $10^{33} cm^{-2}s^{-1}$ can be achieved with a s.c. linac, operated either in pulsed or in cw mode, with optional recirculation, at a total electric wallplug power of order 20 MW. Higher luminosities, of several $10^{33} cm^{-2}s^{-1}$ can be reached by investing more electric power or by energy recovery. Finally, merits of a linac-ring ep collider are discussed.

  5. Status of the RFI Linac Prototype

    Swenson, D A

    2004-01-01

    A prototype of the Rf Focused Interdigital (RFI) linac structure is currently under construction at Linac Systems. The RFI linac structure is basically an interdigital (or Wideröe) linac structure with rf quadrupole focusing incorporated into each drift tube. The 200 MHz RFI prototype, consisting of a short RFQ linac followed by a short RFI linac, will accelerate a 20 mA beam of protons from an injection energy of 25 keV to an output energy of 2.50 MeV in a total linac structure length of 1.44 meters. The linac structures are designed for continuous (cw) operation, and will be tested initially at a 33% duty factor. The peak structure power of 66 kW and peak beam power of 50 kW will be supplied by a 144 kW, 33% duty rf power system. A microwave ion source will supply the proton beam and an articulated Einzel lens will steer and focus the beam into the RFQ aperture. The mechanical design of the linac structures will be presented, the calculated performance will be described, the status of the components will b...

  6. The environmental research programme of the Centro Nacional de Aceleradores, Sevilla (Spain)

    Full text: The Centro Nacional de Aceleradores (National Accelerator Center, CNA), the first and for the moment the only Spanish ion beam analysis (IBA) laboratory, was set up in 1998 in the University of Seville (Spain). This laboratory was created with the aim to fulfill the increasing demand for IBA techniques existing in Spain. This facility is based on a 3 MB pelletron tandem accelerator, which is being used for interdisciplinary studies concerning Material Science, Art, Archaeology, Biology, Medicine, Environmental Science, etc. In addition, the works for a cyclotron laboratory are commencing now. This paper reports on the most recent applications in the field of Environmental Science carried out in our laboratory. Remediation of metal-contaminated soils and waters poses a challenging problem due to its implications in the environment and the human health. A possible solution to this problem is the phytoremediation, i.e. the process of using plants for environmental restoration taking advantage of the ability of certain terrestrial plants to absorb and accumulate metals, removing them from soils and aqueous streams. These plants are called metal hyper accumulators if they accumulate for instance more than 0.01% of Cd, 0.1% of Ni or 1% of Zn per dry weight in their shoots. For example, Cd is readily transported and accumulated in the shoots of several plant species, being a favourable target metal for this technology. In recent works making use of nuclear microscopy techniques, we investigated the sites of metal localization within the leaves of metal hyper accumulator Arabidopsis thaliana, when plants are grown in a cadmium-rich environment, and we proved that cadmium is sequestered within the trichomes on the leaf surface. The Donana Natural Park is an internationally important wetland area of 280,000 ha in the Huelva-Seville-Cadiz triangle in Southern Spain, which includes natural beaches, dunes, pine forests and marshlands as the most relevant habitats. On

  7. Measurement of 236U on the 1 MV AMS system at the Centro Nacional de Aceleradores (CNA)

    In this paper we present the first comprehensive analysis of the 1 MV AMS system at the Centro Nacional de Aceleradores (CNA, Seville, Spain) for 236U studies in environmental samples. In the last years, this radionuclide has become key in the AMS community, due to the very demanding 236U/238U abundance sensitivities required for general applications. As we demonstrate, the AMS system at the CNA is able to achieve sensitivity for the 236U/238U ratio of about 3 × 10−11 despite its compact design. The use of “239Pu”/238U ratio as a proxy for “236U”/235U background correction is proposed and tested with natural samples that were also studied on the 600 kV Tandy AMS system at the ETH Zürich. This correction is significant in the CNA case, due to the low mass resolving power of the low-energy spectrometer and to the lack of a third filter on the high-energy side. With the measurement of reference solutions supplied by the Institute for Reference Materials and Methods (IRMM-075), and reference natural matrixes provided by the International Atomic Energy Agency (IAEA-Soil-6, IAEA-375; 384; 386 and IAEA-RGU), we show that the 1 MV AMS system at the CNA can be routinely used for determinations of anthropogenic 236U at environmental levels

  8. On the measurement of 10Be on the 1 MV compact AMS system at the Centro Nacional de Aceleradores (Spain)

    In this work we present the most recent improvements performed by our group on 10Be measurements on the 1 MV AMS system recently set up at the CNA (Centro Nacional de Aceleradores), in Seville (Spain). Our efforts have been focused on the study of the viability of our system for BeO and BeF- measurements. To achieve this, different standard materials have been measured to demonstrate the reliability of the system for BeO measurements in a wide 10Be/9Be atomic ratio range and several environmental samples have been studied both at the 1 MV AMS CNA facility and at the 6 MV AMS ETH-PSI facility of Zurich to validate our measurements. The results show a good agreement between laboratories. New experiments also have been carried out selecting 1+ and 2+ charge states at the exit of the accelerator and inserting Si3N3.1 foils with different thicknesses to separate 10Be from its isobar, 10B. The influence of each foil on the overall transmission (detected 10Be compared to BeO- injected into the accelerator) and background level was also assessed. In addition some tests were also done to assess the viability of BeF2 and BaBeF4 measurements at our system. Several metal matrices and cathode preparation procedures for BeO samples were investigated to maximize current and cathode lifetime.

  9. Measurement of {sup 236}U on the 1 MV AMS system at the Centro Nacional de Aceleradores (CNA)

    Chamizo, E. [Centro Nacional de Aceleradores (Universidad de Sevilla, Consejo Superior de Investigaciones Científicas, Junta de Andalucía), Thomas Alva Edison 7, 41092 Seville (Spain); Christl, M. [Laboratory of Ion Beam Physics, ETH Zurich, Otto Stern Weg 5, CH-8093 Zurich (Switzerland); Fifield, L.K. [Department of Nuclear Physics, Research School of Physics and Engineering, The Australian National University, ACT 2601 (Australia)

    2015-09-01

    In this paper we present the first comprehensive analysis of the 1 MV AMS system at the Centro Nacional de Aceleradores (CNA, Seville, Spain) for {sup 236}U studies in environmental samples. In the last years, this radionuclide has become key in the AMS community, due to the very demanding {sup 236}U/{sup 238}U abundance sensitivities required for general applications. As we demonstrate, the AMS system at the CNA is able to achieve sensitivity for the {sup 236}U/{sup 238}U ratio of about 3 × 10{sup −11} despite its compact design. The use of “{sup 239}Pu”/{sup 238}U ratio as a proxy for “{sup 236}U”/{sup 235}U background correction is proposed and tested with natural samples that were also studied on the 600 kV Tandy AMS system at the ETH Zürich. This correction is significant in the CNA case, due to the low mass resolving power of the low-energy spectrometer and to the lack of a third filter on the high-energy side. With the measurement of reference solutions supplied by the Institute for Reference Materials and Methods (IRMM-075), and reference natural matrixes provided by the International Atomic Energy Agency (IAEA-Soil-6, IAEA-375; 384; 386 and IAEA-RGU), we show that the 1 MV AMS system at the CNA can be routinely used for determinations of anthropogenic {sup 236}U at environmental levels.

  10. El impacto de la política monetaria y la política fiscal en un modelo de acelerador financiero

    Botero García, Jesús

    2010-01-01

    El presente artículo presenta un modelo sencillo de acelerador financiero, en el que a partir de la solución del problema de optimización intertemporal del flujo de renta del empresario en condiciones de competencia monopolística, es posible evaluar el impacto de dichos descuentos, así como también el impacto de la política monetaria, sobre el stock deseado de capital y la inversión deseada. El modelo es un modelo de equilibrio parcial, pero ilustra adecuadamente la forma como la política mon...

  11. First Tests for the Detection of the LINAC Irradiation Field Using PIN Diodes

    The employment of the technology of semiconductor detectors, in the medical physics environment is of great importance due to its versatility and dependability. In this work we present the first results and the experimental arrangement employed with PIN diodes that are conditioned for the measurement of the field of irradiation of a lineal accelerator (LINAC) used in radiotherapy. In our tests we used a PIN photodiode. In former experiments, this diode presented a response to the intensity of the applied field when it was exposed to an X-ray beam in medical and industrial radiography equipments. This diode is a low cost and easy acquisition one in the field. These characteristics transform it into a serious candidate as detector to be used in electronic arrangements for the detection of radiation fields in radio-therapy with X-rays. Experiments were designed to obtain the response of this diode when it was exposed to X-ray beams of a LINAC used in radiotherapy. Firstly the tests were carried out for a 6 MeV photon beam with a source to surface distance (SSD) of 100 cm, obtaining very encouraging results. We seek to carry out tests for more energy values in order to obtain the energy response of this detector as a radiation sensor device. This device could be applied in the design of working tools, for example, for the quality control in procedures of radiotherapy

  12. Study of characteristics of linac with TWRR

    High power electron linac which is developed by PNC is an electron linac with the TWRR (Traveling Wave Resonant Ring). Some phenomena occurred on our high power test are mentioned. Some important characteristics such as stability and phase characteristic are discussed. (author)

  13. Wake Field Effect Analysis in APT Linac

    Kurennoy, Sergey S.

    1998-01-01

    The 1.7-GeV 100-mA CW proton linac is now under design for the Accelerator Production of Tritium (APT) Project. The APT linac comprises both the normal conducting (below 211 MeV) and superconducting (SC) sections. The high current leads to stringent restrictions on allowable beam losses (

  14. RF linacs for esoteric applications

    Particle accelerators of various types have been considered for many years in terms of their application to national defense. Recently, the Strategic Defense Initiative has focused and emphasized such applications. After appropriate and extensive development, accelerators could fulfill important roles in a defensive-system architecture and could compete effectively with other technologies. A great deal of the required development is engineering. Aspects of the R and D program on rf-linac-based applications are discussed, and potential long-term influences on accelerator technology are outlined

  15. The linac coherent light source

    The Linac Coherent Light Source is a self-amplified spontaneous emission based free electron laser to be built at the Stanford Linear Accelerator Centre by a multi-laboratory collaboration. This facility will provide ultra-short pulses of coherent X-ray radiation with the fundamental harmonic energy tuneable over the energy range of 0.82 to 8.2 keV. In addition to the coherent X-ray radiation, which will have an extremely high peak and average brightness, a continuous spectrum of spontaneous synchrotron radiation (SR) of high brightness will also be produced. The characteristics of the LCLS and its associated radiological issues are discussed. (authors)

  16. Electron beam linac simulations, 1985

    The results of particle simulation studies of electron beam problems for the year 1985 are summarized. Although the main subjects this year were mostly the same as in previous years, namely foilless diodes, accelerating gaps, and beam extraction, a major new element this year was the addition of IFR (ion-focused-regime) channels to the various components of a linac beam line. Of particular interest may be the new results obtained for IFR autoacceleration gaps (relevant to MIMI), and the studies of extraction from a guide magnetic field onto an IFR propagation channel (relevant to RADLAC II). 49 figs., 20 refs

  17. Induction linacs and pulsed power

    Progress in electronic power conversion technology is making possible a new class of induction linacs that can operate at extremely high repetition rates. Advances in insulator technology, pulse forming line design and switching may also lead to a new type of high current accelerator with accelerating gradients at least an order of magnitude greater than those attainable today. The evolution of the induction accelerator pulsed power system will be discussed along with some details of these emerging technologies which are at the frontiers of accelerator technology

  18. Phase scan signature matching for linac tuning

    A relatively simple method for linac tuning has been devised, tested and used on the Alvarez and side coupled linacs. Tank or Module phase is varied over 360 degrees while the phase of signals from strip-line beam monitor is measured. Reference phase is taken from the master oscillator for the linac. Theoretical curves of beam phase versus tank/module phase are matched to the measured curves to determine the tank/module field amplitude and phase, and the input and output betas of the tanks/modules. Early experiments on tanks 4--7 of the Alvarez linac have demonstrated the feasibility of the technique. Recently this method was used for commissioning of the Fermilab upgraded linac

  19. Contributed papers to the 1984 Linac Conference

    The LEP Injector Linacs (LIL) are the first part of the LEP injection chain, and consist of a 200 MeV high current electron linac, followed by a 600 MeV low current electron/positron linac. First a description of the complete machine is presented. Then the accelerating structures are more particularly described. The automatic phasing system which shall be used during the operation of the linacs is also presented together with measurements and tests. At least the front end linac is described, with the instrumentation developped by LAL in order to measure the beam parameters intensity, energy, emittance, bunch length. Main results of the experimental program which took place in 1982 and 1983 are given

  20. Electrodinámica no lineal en gravitación

    Nora Bretón

    2001-01-01

    Full Text Available Se revisan las motivaciones que dieron lugar a la formulación de la teoría de la electrodinámica no lineal de Born-Infeld; así como el acoplamiento de dicho campo con gravitación, descrito por las ecuaciones de Einstein-Born-Infeld, de las que presenta una solución la cual representa el choque de dos ondas electromagnéticas no lineales, cuya interacción, a diferencia del caso lineal, origina un campo gravitacional. Finalmente, se comenta que la geometría que siente un fotón de Born-Infeld y uno de Maxwell no es la misma.

  1. Planetary method to measure the neutrons spectrum in lineal accelerators of medical use

    A novel procedure to measure the neutrons spectrum originated in a lineal accelerator of medical use has been developed. The method uses a passive spectrometer of Bonner spheres. The main advantage of the method is that only requires of a single shot of the accelerator. When this is used around a lineal accelerator is necessary to operate it under the same conditions so many times like the spheres that contain the spectrometer, activity that consumes enough time. The developed procedure consists on situating all the spheres of the spectrometer at the same time and to realize the reading making a single shot. With this method the photo neutrons spectrum produced by a lineal accelerator Varian ix of 15 MV to 100 cm of the isocenter was determined, with the spectrum is determined the total flow and the ambient dose equivalent. (Author)

  2. El Parque Lineal de Palmira, un espacio dinamizador del desarrollo de la ciudad

    Esperanza Forero Sanclemente

    2015-05-01

    Full Text Available El Parque Lineal de Palmira –una ciudad colombiana intermedia situada en el Valle del Cauca–, puede constituir un eje articulador del desarrollo urbano mediante la integración de todos los factores que intervienen en dicho parque, los que son capaces de convertir este espacio público en un lugar estratégico en el ámbito urbano. En este sentido, los actores de la ciudad consideran el Parque Lineal como una posibilidad de desarrollo y de referencia cultural y ambiental crucial en los planes de ordenamiento y desarrollo de la ciudad. El trabajo investigativo se propone encontrar un conjunto de estrategias ambientales, sociales, económicas, culturales e institucionales, que permitan la sostenibilidad del Parque Lineal, a partir de una Investigación Acción Participativa.

  3. Photons and photoneutrons spectra of a Linac of 15 MV

    Using the Monte Carlo code MCNP-5, the photons and photoneutrons spectra generated in the head stock of the lineal accelerator (Linac) Varian of 15 MV of the Cancerology State of Nayarit were determined. For the calculations a heterogeneous head stock was modeled, more compatible with the work conditions. In the center of the head stock a tungsten target was located on a copper support, followed by the flattened filter. The photons and photoneutrons spectra were obtained accelerating electrons and making them collide against the target to produce photons by Bremsstrahlung, these photons were transported inside the head stock and the photons and photoneutrons spectra were calculated in a punctual detector located under the flattened filter and in the isocenter. The spectra were evaluated in punctual detectors that were located in the plane from the isocenter to the long of the X and Y axes each 20 cm, in an equidistant way, up to 2 m, so much in the longitudinal and transversal axes. In the calculations were used histories 5E(6) with the purpose of obtaining smaller uncertainties to 1%. It was found that the photons spectrum in the punctual detector inside the head stock presents a pick of 1.25 MeV in the energy interval of 0.5 and 1.5 MeV, later suffers a filtration and diminishes in asymptote form. This spectrum modifies when the beam reaches the isocenter, diminishing the low energy photons. Inside the head stock the photoneutrons spectrum shows a structure with two picks, one before 1 MeV and other after 1 MeV; this is for effect of the collimators geometry and the distance. Finally an increment of the total neutrons flow to 60 cm of distance of the isocenter on the Y axis was observed, due to the design geometry of the modeling heterogeneous head stock. (Author)

  4. Modelo no lineal con potencial Seno-Gordon para un cristal fotónico unidimensional

    Margarita Franco Ortíz

    2013-06-01

    Full Text Available Se presenta un modelo para un cristal fotónico unidimensional formado por una sucesión de planos constituidos por material no lineal, inmersos en un medio lineal. Se resuelve la ecuación de Schrödinger introduciendo en el hamiltoniano modelo del cristal un potencial no lineal tipo Seno-Gordon. Se obtiene analíticamente una versión generalizada, dependiente de la amplitud de la onda incidente, de la ecuación trascendente que caracteriza al modelo del cristal de Kronig-Penney, de donde se determina la estructura de las bandas de energía del cristal. El modelo puede aplicarse a una versión finita de un cristal fotónico para un número limitado de capas alternadas de material lineal y no lineal para el cual se han calculado la reflectancia como una función de la intensidad de la onda electromagnética, el índice de la banda y el número de períodos. Es posible construir un sistema con estas características alternando capas muy delgadas de material de materia blanda no lineal con capas sólidas más gruesas, con el cual puede diseñarse un dispositivo para controlar la propagación de luz para intervalos de longitudes de onda específicos e intensidades de la luz de la misma señal que se propaga.

  5. Indigenous 6 MV medical LINAC

    Linear Accelerators were made for physics research all over the world; in India too the first indigenous accelerator was made for research of materials using the 3.5 MeV Linear Accelerator in the 1960s at the Tata Institute of Fundamental Research, Mumbai. Prof. R.V.S. Sitaram was the leading scientist who contributed in the development of the first indigenous linac that served research scholars for more than two decades. The travelling wave S-band Linac using a magnetron as a source of high power microwaves was a significant development towards the indigenous accelerator. The accelerating structure had magnetic coils for beam focusing, the HV modulator, microwave system and control unit were indigenously developed by TIFR scientists. Dr. Homi Bhabha, Director, TIFR had taken keen interest in the project and an appropriate room in the basement was selected for the accelerator facility. The Iinac tube cavities, magnetic coils and pulse transformer were designed and fabricated in TIFR laboratory and only raw material was imported. The group working on Radar transmitters developed the transmission line type modulator using components such as charging choke and locally available HV transformers. However, the rectifier diodes, cores switching tubes were imported. The complete system design was done in-house and also included operation and maintenance of the facility. Over its life of two decades, a second generation of technologists were developed with a first hand knowledge of an accelerator system

  6. The DARHT Phase 2 Linac

    Rutkowski, H L; Waldron, W L; Chow, K P; Vella, M C; Fawley, W M; Briggs, R; Nelson, S; Wolf, Z; Birx, D L; Rutkowski, HL; Reginato, LL; Waldron, WL; Chow, KP; Vella, MC; Fawley, WM

    2000-01-01

    The second phase accelerator for the Dual Axis Hydrodynamic Test facility (DARHT) is designed to provide an electron beam pulse that is 2 microsec long, 2kA, and 20 MeV in particle energy. The injector provides 3.2 MeV so that the linac need only provide 16.8 MeV. The linac is made with two types of induction accelerator cells. The first block of 8 cells have a 14 in. beam pipe compared to 10 in. in the remaining 80 cells. The other principal difference is that the first 8 cells have reduced volt-sec in their induction cores as a result of a larger diameter beam pipe. The cells are designed for very reliable high voltage operation. The insulator is Mycalex. Results from prototype tests are given including results from solenoid measurements. Each cell contains a solenoid for beam transport and a set of x-y correction coils to reduce corkscrew motion. Details of tests to determine RF mode impedances relevant to BBU generation are given. Blocks of cells are separated by "intercells" some of which contain transpo...

  7. Una aplicación de MATLAB sobre Programación No Lineal bidimensional

    Fernando Giménez Palomares

    2014-03-01

    Full Text Available La Programación No Lineal (PNL constituye una herramienta de amplia aplicación en la modelización de problemas de la vida real aplicados a los negocios, la economía, la empresa y la ingeniería. Consiste en maximizar o minimizar un campo escalar cuyo dominio viene dado a partir de un conjunto de restricciones dadas por igualdades y/o desigualdades no necesariamente lineales. En este trabajo se presenta un laboratorio virtual que permite estudiar gráfica y numéricamente la PNL en el caso de dos variables.

  8. Una aplicación de MATLAB sobre Programación No Lineal bidimensional

    Fernando Giménez Palomares; María José Marín Fernández

    2014-01-01

    La Programación No Lineal (PNL) constituye una herramienta de amplia aplicación en la modelización de problemas de la vida real aplicados a los negocios, la economía, la empresa y la ingeniería. Consiste en maximizar o minimizar un campo escalar cuyo dominio viene dado a partir de un conjunto de restricciones dadas por igualdades y/o desigualdades no necesariamente lineales. En este trabajo se presenta un laboratorio virtual que permite estudiar gráfica y numéricamente la PNL en el caso de do...

  9. Codis no lineals en MAGMA : construcció de codis perfectes

    Vidal Marín, Laura

    2009-01-01

    La finalitat d'aquest projecte és aconseguir construir codis binaris perfectes no lineals de manera eficient. Per a fer-ho, hem desenvolupat un paquet de software per a l'intèrpret MAGMA que conté funcions per a la construcció de codis perfectes, càlcul d'invariants de codis i altres funcions complementàries per a fer càlculs sobre les paraules d'un codi. La finalidad de este proyecto es conseguir construir códigos binarios perfectos no lineales de forma eficiente. A tal efecto, hemos desa...

  10. IDENTIFICACIÓN DE EPISODIOS DE DEPENDENCIA NO LINEAL EN EL PESO MEXICANO

    Gatica Arreola Leonardo; Coronado Ramírez Semei

    2011-01-01

    El siguiente documento identifica episodios de dependencia no-lineal en el tipo de cambio mexicano (peso mexicano/dólar norteamericano), entre enero de 1995 y septiembre de 2010. Para ello se utiliza la metodología Hinich Portmanteau, la cual utiliza una prueba de alta frecuencia para detectar episodios de dependencia no lineal, por medio de funciones ventana. Se proporciona una explicación de los sucesos económicos y políticos que pudieron haber provocado que el tipo de cambio tuviera un com...

  11. 25th anniversary for Linac-2

    2003-01-01

    On Friday, 3 October 2003, the Linac team celebrated a quarter century of successful operation of one of its linear accelerators: Linac-2, the proton workhorse of the CERN accelerator complex. Linac-2, CERN's linear proton accelerator, has now been running for 25 years - ample reason for a small celebration. About 30 members of the original team (10 of the initially more than 50 are still working at CERN), and other CERN personnel met on 3 October 2003. Linac-2 is the first link in the accelerator chain Linac-2 - PS Booster - PS - SPS and eventually LHC. Beams from Linac-2 are used after further acceleration in the CERN complex for SPS fixed target physics; for antiproton production for the Antiproton Decelerator (AD); for test beams in the East Experimental Hall and in the PS; for nuclear physics at ISOLDE; for LHC test beams and in the past for both ISR physics and Antiproton production (AA/AC) and test beams in LEAR. Linac-2 was built to obtain higher intensities and better stability than with ...

  12. PACIENTES PORTADORAS DE CÂNCER DE MAMA, SUBMETIDAS À RADIOTERAPIA COM ACELERADOR LINEAR E QUALIDADE DE VIDA

    Lívia Almeida Fortunato

    2015-12-01

    Full Text Available A radioterapia é um tratamento eficaz contra o câncer de mama que tem a finalidade de destruir as células neoplásicas. Entretanto, pode produzir efeitos adversos causando alterações importantes na qualidade de vida (QV das pacientes durante e após o tratamento. Assim, essa pesquisa que tem por objetivo comparar a qualidade de vida de mulheres com câncer de mama no início e após se submeterem a radioterapia com acelerador linear. O estudo foi realizado no hospital denominado OncoBeda, na cidade de Campos dos Goytacazes - RJ. A amostra foi composta por 20 pacientes do gênero feminino, com idade entre 33 a 87 anos. As mesmas responderam nos momentos pré e pós tratamento ao Instrumento WHOQOL-bref, composto por 26 questões, sendo 2 questões gerais sobre auto avaliação da QV e as outras 24 questões que envolvem 4 domínios, sendo eles “físico”, “psicológico”, “relações sociais” e “meio ambiente”. Os resultados obtidos revelam que houve uma diferença ligeiramente significativa no domínio “físico”, influenciando na avaliação geral da QV dessas pacientes. Sendo assim, conclui-se que mesmo não tendo um valor elevado de diferença entre os dois momentos avaliados, as pacientes apresentaram alteração na sua QV durante o tratamento.

  13. Wire alignment system for ATF LINAC

    A wire based alignment system is adopted to make less than 40μm precision alignment for injector linac of Accelerator Test Facility (ATF). The system consists of two stretched SUS wires, pickup coils and active mover stages. The position of pickup coils in a mount which will be installed into LINAC stages is set to the calculated wire position prior to installation. All of LINAC stages are then moved to keep the calculated position by the active mover. The test results of wire position detection in a long term are described. (author)

  14. The SNS super conducting linac architecture

    A new Spallation Neutron Source (SNS) is presently under construction at the Oak Ridge National Laboratory in Tennessee. A conventional linac, accelerates a 52-mA beam to 186 MeV. The SRF linac accelerates the beam to 1.25 GeV using 117 elliptically shaped 6 cell cavities. Two cavity beta types are used, with geometrical betas of 0.61 and 0.81. This paper describes the optimization leading to the choice of cavity betas and number of different cavity types. Also, beam-dynamics throughout the entire linac are presented. (author)

  15. Superconducting LINAC booster for the Mumbai pelletron

    B Srinivasan; S K Singh; R G Pillay; M P Kurup; M K Pandey

    2001-08-01

    We are in the process of constructing a superconducting linear accelerator (LINAC), to boost the energy of heavy ion beams from the 14UD Pelletron accelerator, at Tata Institute of Fundamental Research, Mumbai. The accelerating structures in the LINAC are quarter wave resonators (QWR) coated with lead which is superconducting at liquid helium temperature. With feasibility studies having been completed during the course of the 4th and 5th five-year plan periods, culminating with the demonstration of beam acceleration using one accelerating module, the construction of the LINAC is now under way.

  16. Linac Upgrades for FERMI@ELETTRA

    D'Auria, G; Craievich, P; De Ninno, G; Di Mitri, S; Ferianis, M; Pangon, G; Rumiz, R L; Tosi, T L; Zangrando, D

    2004-01-01

    To fulfill the stringent requirements expected from the FERMI project, the existing Linac needs some modifications in the layout and an upgrading of the present plants. Moreover, for the next two years, until the new injection system (now under construction) is fully commissioned, the Linac has to be kept in operation as injector for the ELETTRA Storage Ring. Therefore most of the planned activities have to be carried out without interfering with the normal operation of the machine. Details on the new Linac layout and related activities are discussed.

  17. The superconducting linac booster at the ANU

    This report outlines the progress of the installation of the superconducting Linac booster at the Australian National University. The Linac is based upon four modules, three of which contain three split-loop resonators. The fourth cryostat was intended to be a superbuncher and so houses only one resonator. The first stage of Linac operation will employ only three modules with 2 MV/m from each resonator. It is expected that the implementation of all nine modules, in subsequent stages, would boost beams by 18 MV/q. The project has fostered productive international collaboration between UK and Australian scientists. 1 tab., 6 figs

  18. A novel electron gun for inline MRI-linac configurations

    Constantin, Dragoş E.; Holloway, Lois; Keall, Paul J.; Fahrig, Rebecca

    2014-01-01

    Purpose: This work introduces a new electron gun geometry capable of robust functioning in the presence of a high strength external magnetic field for axisymmetric magnetic resonance imaging (MRI)-linac configurations. This allows an inline MRI-linac to operate without the need to isolate the linear accelerator (linac) using a magnetic shield. This MRI-linac integration approach not only leaves the magnet homogeneity unchanged but also provides the linac flexibility to move along the magnet a...

  19. Modeling of the ALS linac

    The ALS injector linac is used for the Beam Test Facility (BTF) and the Damping Experiments when it is available in between the ALS filings. These experiments usually require higher quality beams and a better characterization than is normally required for ALS operations. This paper focuses on the beam emittance, energy tilt, and especially the longitudinal variation of the beam parameters. For instance, the authors want to avoid longitudinal variations at the low beta section of the BTF. On the other hand, a large energy tilt is required for post-acceleration compression of the bunch using an alpha magnet. The PARMELA code was modified to calculate and display longitudinal variations of the emittance ellipse. Using the Microsoft Development Studio under Windows NT environment the code can handle a much larger number of particles than was previously possible

  20. Symmetry properties of lineal operator eigenfunctions defined in bidimensional systems. Application to uniform and homogeneous wavequides

    Symmetry properties of the eigenfunctions of lineal operators, associated to bidimensional problems with rotational or reflection symmetries, are analyzed by means of a simple systematic approach which does not have recourse to the usual group theory. An application to the determination of the symmetry properties of electromagnetic waveguides modes, associated to uniform transmission systems, is presented. (author)

  1. Estabilidad y convergencia de esquemas numéricos para sistemas de Dirac no lineales

    Frutos, J. de

    1989-01-01

    Siguiendo una técnica desarrollada por López-Marcos y Sanz-Serna, probamos la estabilidad y convergencia de tres esquenias en diferencias finitas para la solución numérica de sistemas de Dirac no lineales. Los esquemas se comparan por medio de experimentos numéricos. Peer Reviewed

  2. Operational experience with the CERN hadron linacs

    The present CERN proton linac (Linac2) was commissioned in 1978 and since that date has been the primary source of protons to the CERN accelerator complex. During the past 18 years, the machine has had a very good reliability record in spite of the demands made upon it. Modifications have been made with the view of maintaining this reliability with reduced resources and new requirements from the users. Further demands will be made in the future for LHC operation. In 1994, a new linac for heavy ion production was put into service replacing the original CERN proton linac. As this machine was built within an international collaboration, operation had to take into account the novelty of the techniques used and the variety of equipment supplied by outside collaborators. Even so, the new machine has also had very good reliability. (author)

  3. The invention that is shaping Linac4

    CERN Bulletin

    2010-01-01

    Accelerator experts are no strangers to innovative optimizations of existing techniques and to the development of novel solutions. Sometimes, they even come up with ideas that have the potential to revolutionize the field. This is the case with the Tolerance Aligned Cantilever Mounting (TACM) system, a completely new way of supporting the drift tubes, one of the core elements of linear accelerators. The new, patent-pending technique will be implemented at Linac4.   Drift tubes in a prototype for Linac4, assembled using the new TACM technology. “Assemble and adjust” – that was the technique used to build drift-tube linacs before the arrival of the TACM. Now, the inventors’ motto has become ‘adjust and assemble’. The inversion of these two words represents a real revolution for people working in the field. “The drift tubes are a critical element of Linac4 and they have to satisfy several requirements: they have to be mechanically ...

  4. Progress in the photocathode linac project

    The progress achieved so far in the Photocathode Linac Project have developed and tested linear accelerator structures at 2856 MHz, commissioned the klystron modulator and microwave systems, and developed the beamline, and are ready to commence acceleration experiments

  5. BLIP. [Brookhaven Linac Isotope Producer (BLIP)

    Stang, Jr, L G

    1976-01-01

    The operation of the Brookhaven Linac Isotope Producer (BLIP) is discussed. Topics covered include targets, target holders, linac specifications, beam transport, and current production performance. The use of the BLIP is confined exclusively to the development of radionuclides that are, or should be, of medical interest, and the facility is moving rapidly into a self-supporting state from the income of the products. (PMA)

  6. Generación de modelos de enseñanza–aprendizaje en álgebra lineal

    Miranda , Eduardo

    2004-01-01

    Dos de las dificultades más importantes y frecuentes que encontramos en el aprendizaje del álgebra lineal, tenemos la conceptualización y la formalización. Los contenidos de la materia son, en gran medida, formulados a partir de la definición de vectores, espacios vectoriales, bases, transformaciones lineales, etc. En los primeros capítulos de un curso de álgebra lineal, es frecuente acudir a la visualización geométrica en R2 y R3 como ayuda pedagógica para ilustrar las representaciones vecto...

  7. Physics design of the National Spallation Neutron Source linac

    The National Spallation Neutron Source (NSNS) requires a linac that accelerates a H- beam to 1.0 GeV. The linac starts with a radio-frequency quadrupole (RFQ) accelerator, which is followed by a drift-tube linac (DTL), a coupled-cavity drift-tube linac (CCDTL), and a conventional coupled-cavity linac (CCL). In this paper, the authors focus on the DTL, CCDTL, and CCL parts of the accelerator. They discuss the linac design parameters and beam dynamics issues. The design rationale of no separate matching sections between different accelerating sections maintains the current independence of beam behavior

  8. Linac4 H- ion sources

    Lettry, J.; Aguglia, D.; Alessi, J.; Andersson, P.; Bertolo, S.; Briefi, S.; Butterworth, A.; Coutron, Y.; Dallocchio, A.; David, N.; Chaudet, E.; Faircloth, D.; Fantz, U.; Fink, D. A.; Garlasche, M.; Grudiev, A.; Guida, R.; Hansen, J.; Haase, M.; Hatayama, A.; Jones, A.; Koszar, I.; Lallement, J.-B.; Lombardi, A. M.; Machado, C.; Mastrostefano, C.; Mathot, S.; Mattei, S.; Moyret, P.; Nisbet, D.; Nishida, K.; O'Neil, M.; Paoluzzi, M.; Scrivens, R.; Shibata, T.; Steyaert, D.; Thaus, N.; Voulgarakis, G.

    2016-02-01

    CERN's 160 MeV H- linear accelerator (Linac4) is a key constituent of the injector chain upgrade of the Large Hadron Collider that is being installed and commissioned. A cesiated surface ion source prototype is being tested and has delivered a beam intensity of 45 mA within an emittance of 0.3 π ṡ mm ṡ mrad. The optimum ratio of the co-extracted electron- to ion-current is below 1 and the best production efficiency, defined as the ratio of the beam current to the 2 MHz RF-power transmitted to the plasma, reached 1.1 mA/kW. The H- source prototype and the first tests of the new ion source optics, electron-dump, and front end developed to minimize the beam emittance are presented. A temperature regulated magnetron H- source developed by the Brookhaven National Laboratory was built at CERN. The first tests of the magnetron operated at 0.8 Hz repetition rate are described.

  9. The Linac Coherent Light Source

    A collaboration of scientists from SLAC, UCLA, Los Alamos National Laboratory, Brookhaven National Laboratory, and Argonne National Laboratory have proposed to build the Linac Coherent Light Source (LCLS) facility, a free-electron laser (FEL) on the SLAC site, spanning photon energies 0.8-8 keV. The laser output will be 8-10 GW with pulse lengths 230 fsec or less. The LCLS will offer unprecedented experimental opportunities in the areas of atomic physics, chemical dynamics, plasma physics, nanoscale dynamics, and biomolecular imaging. SLAC has proposed to begin engineering design of the laser in 2003, leading to project completion in 2008. The laser produces x-rays by the self-amplified spontaneous emission (SASE) process: an intense, highly collimated pulse of 14.5 GeV electrons, traveling through a 122 m-long undulator magnet system, is induced by its own synchrotron radiation to form sub-nanometer-scale bunches. The bunching process enhances the coherence and hence the intensity of the emitted synchrotron radiation. The process is analogous to the instability of a high-gain amplifier; the ''noise'' signal that seeds the instability is the shot noise in the electron beam

  10. Linac4 H⁻ ion sources.

    Lettry, J; Aguglia, D; Alessi, J; Andersson, P; Bertolo, S; Briefi, S; Butterworth, A; Coutron, Y; Dallocchio, A; David, N; Chaudet, E; Faircloth, D; Fantz, U; Fink, D A; Garlasche, M; Grudiev, A; Guida, R; Hansen, J; Haase, M; Hatayama, A; Jones, A; Koszar, I; Lallement, J-B; Lombardi, A M; Machado, C; Mastrostefano, C; Mathot, S; Mattei, S; Moyret, P; Nisbet, D; Nishida, K; O'Neil, M; Paoluzzi, M; Scrivens, R; Shibata, T; Steyaert, D; Thaus, N; Voulgarakis, G

    2016-02-01

    CERN's 160 MeV H(-) linear accelerator (Linac4) is a key constituent of the injector chain upgrade of the Large Hadron Collider that is being installed and commissioned. A cesiated surface ion source prototype is being tested and has delivered a beam intensity of 45 mA within an emittance of 0.3 π ⋅ mm ⋅ mrad. The optimum ratio of the co-extracted electron- to ion-current is below 1 and the best production efficiency, defined as the ratio of the beam current to the 2 MHz RF-power transmitted to the plasma, reached 1.1 mA/kW. The H(-) source prototype and the first tests of the new ion source optics, electron-dump, and front end developed to minimize the beam emittance are presented. A temperature regulated magnetron H(-) source developed by the Brookhaven National Laboratory was built at CERN. The first tests of the magnetron operated at 0.8 Hz repetition rate are described. PMID:26932021

  11. Klystron pulse mudulator for linac

    A highly stable klystron pulse modulator is required in constructing a linac with good beam characteristics. The De-Qing circuit has been used conventionally to stabilize the output of a pulse modulator, but this method can achieve a stability of 1 percent at best, which is far larger than the targeted stability (less than 0.1 percent). The following three types of regulators are available to stabilize the D.C. power source of a pulse modulator: series regulator, shunt regulator and switching regulator. Advantages and disadvantages of these regulators are examined and the shunt regulator is selected because of its simple circuit structure and easy adjustment. The klystron pulse modulator has the features of being able to serve as a component of a large-power pulse klystron, being high in pulse stability (reproducibility), giving good pulse profiles (free from evershoot or undershoot), being small in size, etc. The klystron pulse modulator consists of a power source step-up transfermer, three-phase full-wave rectifying circuit, smoothing circuit, constant voltage control circuit, switching circuit, PFN circuit and pulse transformer. (Nogami, K.)

  12. RNB-specific linac development

    Ratzinger, U

    2002-01-01

    The acceleration of secondary, radioactive beams from primary beam driven ion sources provides many challenges when compared to the case of conventional ion beams. The clean separation of the specific ion species, the low beam current, the short life time of the ions as well as the needed energy variability have consequences on the layout of the accelerator. As also experiments with astrophysical relevance are performed, the energy range should go down below 1 MeV/u in some cases. Additionally, to investigate nuclear reactions around the Coulomb barrier, the beam energy should be flexible up to around 8 MeV/u. Short isotope life times below a few milliseconds do not allow for charge breeding. In these cases, low charged ions from 'simple' ion sources have to be accepted by the accelerator. Furthermore, stripping processes along the linac are excluded in case of low beam currents. Multicoincidence experiments profit a lot from cw operation of ion source and accelerators. During the last three decades, room tem...

  13. CERN Linac4. The space charge challenge

    Hein, Lutz Matthias

    2013-08-06

    In the first phase of the upgrade program of the CERN accelerator complex the proton injector Linac2 will be replaced by a new, normal-conducting H-ion Linac, Linac4, allowing a significant increase of the proton flux intensity along the downstream accelerator complex. In the design of Linac4 three beam transport sections are implemented to match the beam between the different accelerator elements and to model the longitudinal pulse structure. These three beam transport sections, which are the most critical locations in terms of beam quality preservation, are in the focus of this thesis. During the work of this thesis the Low Energy Beam Transport (LEBT), which is required to match the source beam to the radiofrequency quadrupole (RFQ), has been commissioned and its beam dynamics re-constructed. The measurement campaign used to reconstruct the LEBT beam dynamics was performed with the aim to prepare the RFQ commissioning and to maximise the LEBT performance. Downstream of the Linac4 accelerator the beam is transported along a 180 m long transfer line to the Proton Synchrotron Booster (PS-Booster). The transfer line optics was studied, optimised and sections were completely re-designed. The new transfer line optics is characterised by an improved preservation of the beam emittance, higher stability of the optical solution with respect to alignment errors and field jitters of the transfer line magnets and it is matched to each of the PS-Booster injection schemes. In a concluding ''Start-To-End'' simulation based on the measured beam characteristics at the LEBT exit the beam dynamics of the downstream Linac, including the transfer line, was calculated. To minimise particle losses within acceptable emittance preservation the beam optics of the Medium Energy Beam Transport (MEBT) was adapted to the measured beam parameters. This ''Start-To-End'' simulation was performed to identify critical sections of the Linac4 beam dynamics and

  14. CERN Linac4. The space charge challenge

    In the first phase of the upgrade program of the CERN accelerator complex the proton injector Linac2 will be replaced by a new, normal-conducting H-ion Linac, Linac4, allowing a significant increase of the proton flux intensity along the downstream accelerator complex. In the design of Linac4 three beam transport sections are implemented to match the beam between the different accelerator elements and to model the longitudinal pulse structure. These three beam transport sections, which are the most critical locations in terms of beam quality preservation, are in the focus of this thesis. During the work of this thesis the Low Energy Beam Transport (LEBT), which is required to match the source beam to the radiofrequency quadrupole (RFQ), has been commissioned and its beam dynamics re-constructed. The measurement campaign used to reconstruct the LEBT beam dynamics was performed with the aim to prepare the RFQ commissioning and to maximise the LEBT performance. Downstream of the Linac4 accelerator the beam is transported along a 180 m long transfer line to the Proton Synchrotron Booster (PS-Booster). The transfer line optics was studied, optimised and sections were completely re-designed. The new transfer line optics is characterised by an improved preservation of the beam emittance, higher stability of the optical solution with respect to alignment errors and field jitters of the transfer line magnets and it is matched to each of the PS-Booster injection schemes. In a concluding ''Start-To-End'' simulation based on the measured beam characteristics at the LEBT exit the beam dynamics of the downstream Linac, including the transfer line, was calculated. To minimise particle losses within acceptable emittance preservation the beam optics of the Medium Energy Beam Transport (MEBT) was adapted to the measured beam parameters. This ''Start-To-End'' simulation was performed to identify critical sections of the Linac4 beam dynamics and to adjust the commissioning strategies.

  15. ROPAX 1200 pasajeros, 5000 metros lineales para trailers y 11500 TPM.

    Valea Peces, Álvaro

    2016-01-01

    Ferry de día - ROPAX para 1200 pasajeros distribuidos en 300 camarotes cuádruples con aseo y espacios públicos a razón de 3.5 m2 por persona. Tiene una capacidad de carga de 5000 metros lineales para trailers y 230 metros lineales para coches (carga simultánea), para un total de 11500 toneladas de peso muerto. El buque contará con portalón de popa y proa (double enter). La velocidad en pruebas será de 22 nudos al 85% MCR y se tomará un margen de mar del 15%. La autonomía será de 3000 millas...

  16. Transformaciones lineales. Una mirada desde la teoría APOE

    Maturana, Isabel; Parraguez, Marcela

    2013-01-01

    El artículo que presentamos a continuación corresponde a una investigación en proceso en didáctica de la matemática relacionada al concepto de transformación lineal; bajo la teoría APOE como marco teórico y un diseño metodológico correspondiente a un estudio de caso múltiple. A partir de esta investigación se obtendrá documentación sobre el esquema del concepto Transformación Lineal reconociendo tres interpretación en este, es decir interpretación matricial- interpretación geométrica – e inte...

  17. Monte Carlo simulations of the cellular S-value, lineal energy and RBE for BNCT

    Due to the non-uniform uptake of boron-containing pharmaceuticals in cells and the short-ranged alpha and lithium particles, microdosimetry provides useful information on the cellular dose and response of boron neutron capture therapy (BNCT). Radiation dose and quality in BNCT may be expressed in terms of the cellular S-value and the lineal energy spectrum. In the present work, Monte Carlo simulations were performed to calculate these microdosimetric parameters for different source-target configurations and sizes in cells. The effective relative biological effectiveness (RBE) of the Tsing Hua Open-pool Reactor (THOR) epithermal neutron beam was evaluated using biological weighting functions that depended on the lineal energy. RBE changes with source-target configurations and sizes were analyzed. (author)

  18. Radiosurgery with a linear accelerator in cerebral arteriovenous malformations Radiocirurgia com acelerador linear em malformações arteriovenosas cerebrais

    Sérgio Carlos Barros Esteves

    2008-04-01

    variables no statistically significant correlation was observed between occlusion and treatment complications.OBJETIVO: Analisar os resultados obtidos com radiocirurgia e as suas complicações do procedimento, no tratamento das malformações arteriovenosas com acelerador linear. MÉTODOS: Este é um estudo retrospectivo. Entre Outubro de 93 e Dezembro de 96, sessenta e um pacientes com malformações arteriovenosas foram tratados, utilizando um acelerador linear com 6MV de energia. As idades variaram de 6 a 54 anos (média: 28,3 anos, 32 pacientes mulheres e 29 pacientes homens. O sintoma inicial mais freqüente foi cefaléia (45,9%, seguido de déficit neurológico (36,1%. Hemorragia cerebral diagnostica por exame de imagem foi observada em 35 pacientes (57,3%. A maioria das malformações arteriovenosas (67,2% eram graus III e IV de Spetzler. Estenose venosa (21,3% e aneurisma (13,1% foram as mais freqüentes alterações da arquitetura vascular. A dose administrada variou de 12 a 27,5Gy na periferia da lesão. RESULTADOS: Dos vinte e oito pacientes que se submeteram a controle angiográfico conclusivo, 18 tiveram obliteração completa (72% e 7 falharam ao tratamento (ausência de oclusão com mais de três anos de seguimento. Quatro pacientes foram submetidos a uma segunda radiocirurgia, e um paciente deste grupo apresentou obliteração em 18 meses de seguimento. DISCUSSÃO: Vários fatores foram analisados em relação ao grau de oclusão (sexo, idade, volume, localização, Spetzler, fluxo, embolização, total de isocentros, dose prescrita e isodose escolhida e complicações (total de isocentros, localização, volume, dose máxima, dose prescrita e isodose escolhida. As variáveis analisadas não mostraram significância estatística para a obliteração do vaso, bem como para as complicações de tratamento. O maior diâmetro da malformação arteriovenosa, seu volume e a dose administrada não influenciaram no tempo de obliteração. CONCLUSÃO: Radiocirurgia

  19. Dispersion and betatron matching into the linac

    In high energy linear colliders, the low emittance beam from a damping ring has to be preserved all the way to the linac, in the linac and to the interaction point. In particular, the Ring-To-Linac (RTL) section of the SLAC Linear Collider (SLC) should provide an exact betatron and dispersion match from the damping ring to the linac. A beam with a non-zero dispersion shows up immediately as an increased emittance, while with a betatron mismatch the beam filaments in the linac. Experimental tests and tuning procedures have shown that the linearized beta matching algorithms are insufficient if the actual transport line has some unknown errors not included in the model. Also, adjusting quadrupole strengths steers the beam if it is offset in the quadrupole magnets. These and other effects have lead to a lengthy tuning process, which in the end improves the matching, but is not optimal. Different ideas will be discussed which should improve this matching procedure and make it a more reliable, faster and simpler process. 5 refs., 2 figs

  20. RFI-Based Ion Linac Systems

    Swenson, Donald A.

    A new company, Ion Linac Systems, Inc., has been formed to promote the development, manufacture, and marketing of intense, RFI-based, Ion Linac Systems. The Rf Focused Interdigital (RFI) linac structure was invented by the author while at Linac Systems, LLC. The first step, for the new company, will be to correct a flaw in an existing RFI-based linac system and to demonstrate "good transmission" through the system. The existing system, aimed at the BNCT medical application, is designed to produce a beam of 2.5 MeV protons with an average beam current of 20 mA. In conjunction with a lithium target, it will produce an intense beam of epithermal neutrons. This system is very efficient, requiring only 180 kW of rf power to produce a 50 kW proton beam. In addition to the BNCT medical application, the RFI-based systems should represent a powerful neutron generator for homeland security, defence applications, cargo container inspection, and contraband detection. The timescale to the demonstration of "good transmission" is early fall of this year. Our website is www.ionlinacs.com.

  1. Métodos numéricos para problemas no lineales

    Ferragut Canals, Luis

    2012-01-01

    En la monografía se tratan problemas no lineales asociados a operadores monótonos eventualmente multívocos y sus correspondientes inecuaciones asociadas. Se consideran ejemplos que aparecen en aplicaciones a la física e ingeniería. Se estudia su aproximación numérica y la convergencia de distintos algoritmos numéricos algoritmos numéricos para la resolución efectiva sobre ordenador.

  2. Sobre conjuntos s_h de vectores binarios y códigos lineales

    Gómez, Carlos Alexis; Trujillo, Carlos Alberto

    2011-01-01

    Un subconjunto $\\mathcal{A}$ de un grupo conmutativo $G$ notado aditivamente, es un conjunto $S_h$ en $G$, si todas las sumas de $h$ elementos distintos de $\\mathcal{A}$, omitiendo las permutaciones de los sumandos, determinan elementos diferentes en $G$. En este artículo se muestra una relación entre conjuntos $S_h$ en $\\mathbb{F}_{2}^{r}$ y códigos binarios lineales.

  3. Effects of machine errors on the ILC main linac

    王逗; 高杰

    2011-01-01

    For a practical linac, the beam property is affected seriously by any machine imperfections. In this paper, the effects of several main errors in the ILC main linac, such as quadrupole misalignment, magnet strength error and cavity misalignment, were stud

  4. Magnetron based high energy S-band linac system

    This paper deals with the study of magnetron based high energy S-band linear accelerator (linac) system operating at spot frequency 2.998 GHz. The energy and dose are two important parameters of linac system which depend on input power of microwave source and length of linac tube. Here the author has studied how these parameters can be improved for side coupled standing wave S-band linac system

  5. Electro neutrons around a 12 MV Linac

    Neutron contamination around Linacs for radiotherapy is a source of undesirable doses for the patient. The main source of these neutrons is the photonuclear reactions occurring in the Linac head and the patient body. Electrons also produce neutrons through (e, en) reactions. This reaction is known as electro disintegration and is carried out by the electron scattering that produce a virtual photon that is absorbed by the scattering nucleus producing the reaction e + A → (A-1) + n + e'. In this work the electron-neutron spectrum to 100 cm from the isocenter of a 12 MV Linac has been measured using a passive Bonner spheres spectrometer in a novel procedure named Planetary mode. (Author)

  6. Electro neutrons around a 12 MV Linac

    Vega C, H. R. [Universidad Autonoma de Zacatecas, Unidad Academica de Estudios Nucleares, Apdo. Postal 336, 98000 Zacatecas (Mexico); Perez L, L. H., E-mail: fermineutron@yahoo.com [Instituto Zacatecano del Tumor, A. C., Lago de la Encantada No. 294, Fracc. Lomas del Lago, Zacatecas (Mexico)

    2012-10-15

    Neutron contamination around Linacs for radiotherapy is a source of undesirable doses for the patient. The main source of these neutrons is the photonuclear reactions occurring in the Linac head and the patient body. Electrons also produce neutrons through (e, en) reactions. This reaction is known as electro disintegration and is carried out by the electron scattering that produce a virtual photon that is absorbed by the scattering nucleus producing the reaction e + A {yields} (A-1) + n + e'. In this work the electron-neutron spectrum to 100 cm from the isocenter of a 12 MV Linac has been measured using a passive Bonner spheres spectrometer in a novel procedure named Planetary mode. (Author)

  7. Required energy gain in the linac

    Sheppard, J.C.

    1985-05-01

    The purpose of this note is to determine how much energy is required for each bunch at the end of the linac such that 100 GeV center of mass collision energy at the IP may be achieved. Once this has been ascertained it is possible to decide how much energy per station in the linac is needed, considering the effects of beamloading, shortened pieces of DLWG, and RF detuning. An appendix is included to cover a related topic: assuming lower bunch currents and lower collision energies, how many low power klystrons can remain in the linac. An attempt has been made to indicate what assumptions have been made so that the readers may try other assumptions to see what happens.

  8. Beam steering in the SLC linac

    In order to control emittance growth due to transverse wakefields it will be necessary to transport electrons and positrons through the Stanford Linear Collider (SLC) linac to within a hundred μm of the centers of the linac irises. Beam centering will be accomplished using computer routines to read stripline beam position monitors and in turn correct the orbits with dipole magnets. Several different steering algorithms have been investigated using electrons in the first third of the SLC linac lattice. The most promising scheme is a cascade of modified ''three-bumps'' in conjunction with long spanning harmonic corrections. General features of the orbit correcting software are discussed along with the mathematical recipes for correction. Experimental results and a discussion of future plans are presented

  9. System design work on proton linac

    The Neutron Science Project at JAERI calls for a high intensity proton linear accelerator with an energy of 1.5 GeV and an average beam power of 8 MW. The linac is required to operate in both pulse (up to 30% duty factor) and CW mode. The front end part of the linac, which consists of an RFQ, a DTL and an SDTL (Separated type DTL), uses normal conducting structures. The higher energy structure is superconducting (SC). The system design and beam dynamics studies have been performed with the PARMTEQ and modified PARMILA codes. An equipartitioned design approach has been taken for the DTL, the SDTL and the SC sections to obtain lower longitudinal emittance growth. The linac design parameters and the beam simulation results are presented. (J.P.N.)

  10. The Linac Coherent Light Source (LCLS) Accelerator

    The Linac Coherent Light Source (LCLS) is a SASE x-ray Free-Electron Laser (FEL) based on the final kilometer of the Stanford Linear Accelerator. Such an FEL requires a high energy, high brightness electron beam to drive the FEL instability to saturation. When fed by an RF-photocathode gun, and modified to include two bunch compressor chicanes, the SLAC linac will provide such a high quality beam at 14 GeV and 1-(micro)m normalized emittance. In this paper, we report on recent linac studies, including beam stability and tolerances, longitudinal and transverse feedback systems, conventional and time-resolved diagnostics, and beam collimation systems. Construction and installation of the injector through first bunch compressor will be completed by December 2006, and electron commissioning is scheduled to begin in January of 2007

  11. Intense positron beams: linacs - preworkshop copy

    Beams of monoenergetic positrons with energies of a few eV to many keV have been used in experiments in atomic physics, solid-state physics and materials science. The production of positron beams from a new source, an electron linac, is described. Intense, pulsed beams of low-energy positrons have been produced by a high-energy beam from an electron linac. The production efficiency, moderator geometry, beam spot size and other positron beam parameters have been determined for electrons with energies from 60 to 120 MeV. Low-energy positron beams produced with a high-energy electron linac can be of much higher intensity than those beams currently derived from radioactive sources. These higher-intensity beams will make possible positron experiments previously infeasible

  12. Intense positron beams: linacs. Preworkshop copy

    Beams of monoenergetic positrons with energies of a few eV to many keV have been used in experiments in atomic physics, solid state physics and materials science. The production of positron beams from a new source, an electron linac, is described. Intense, pulsed beams of low-energy positrons have been produced by a high-energy beam from an electron linac. The production efficiency, moderator geometry, beam spot size and other positron beam parameters have been determined for electrons with energies from 60 to 120 MeV. Low-energy positron beams produced with a high-energy electron linac can be of much higher intensity than those beams currently derived from radioactive sources. These higher intensity beams will make possible positron experiments previously infeasible

  13. Transverse Matching Techniques for the SNS Linac

    Jeon Dong Oh; Danilov, Viatcheslav V

    2005-01-01

    It is crucial to minimize beam loss and machine activation by obtaining optimal transverse matching for a high-intensity linear accelerator such as the Spallation Neutron Source linac. For matching the Drift Tube Linac (DTL) to Coupled Cavity Linac (CCL), there are four wire-scanners installed in series in CCL module 1 as proposed by the author.* A series of measurements was conducted to minimize envelope breathing and the results are presented here. As an independent approach, Chu et al is developing an application based on another technique by estimating rms emittance using the wire scanner profile data.** For matching the Medium Energy Beam Transport Line to the DTL, a technique of minimizing rms emittance was used and emittance data show that tail is minimized as well.

  14. The Linac Cooherent Light Source (LCLS) Accelerator

    Wu, Juhao; Emma, P.; /SLAC

    2007-03-21

    The Linac Coherent Light Source (LCLS) is a SASE x-ray Free-Electron Laser (FEL) based on the final kilometer of the Stanford Linear Accelerator. Such an FEL requires a high energy, high brightness electron beam to drive the FEL instability to saturation. When fed by an RF-photocathode gun, and modified to include two bunch compressor chicanes, the SLAC linac will provide such a high quality beam at 14 GeV and 1-{micro}m normalized emittance. In this paper, we report on recent linac studies, including beam stability and tolerances, longitudinal and transverse feedback systems, conventional and time-resolved diagnostics, and beam collimation systems. Construction and installation of the injector through first bunch compressor will be completed by December 2006, and electron commissioning is scheduled to begin in January of 2007.

  15. Drive linac for the Argonne Wakefield Accelerator

    Chojnacki, E.; Konecny, R.; Rosing, M.; Simpson, J.

    1993-08-01

    The drive linac in Phase I of the Argonne Wakefield Accelerator (AWA) will be used to accelerate short duration (10 ps), high charge (100 nC) electron bunches from 2 MV to 20 MV for use in a variety of wakefield acceleration and measurement studies. The high charge is required since this drive bunch will generate the wakefields of interest in various test sections and their amplitudes are proportional to bunch charge. The short bunch duration is required to drive high-frequency wakefields without intra-bunch cancellation effects. The drive linac design was a balance between having a small wake function to maintain a drive bunch energy spread of {le}10% and obtaining an adequate accelerating gradient of {ge}10 MV/m. This yielded a large aperture, low shunt impedance, high group velocity, L-band, standing-wave linac. Details of the design, fabrication, and testing are presented in the following.

  16. Status of the TOP Linac project

    Cianfarani, Cesidio [ENEA, Via E. Fermi 45, Frascati (Rome) (Italy); Cisbani, Evaristo [ISS, Viale Regina Elena 199, Rome (Italy); Orlandi, Gianluca [ENEA, Via E. Fermi 45, Frascati (Rome) (Italy); Frullani, Salvatore [ISS, Viale Regina Elena 199, Rome (Italy); Picardi, Luigi [ENEA, Via E. Fermi 45, Frascatim(Rome) (Italy)]. E-mail: picardi@frascati.enea.it; Concetta Ronsivalle [ENEA, Via E. Fermi 45, Frascati (Rome) (Italy)

    2006-06-23

    The TOP Linac (Oncological Therapy with Protons), under development by ENEA and ISS is a sequence of three pulsed (5 {mu}s 300 Hz) linear accelerators: a 7 MeV, 425 MHz RFQ+DTL (AccSys Model PL-7), a 7-65 MeV, 2998 MHz Side Coupled Drift Tube Linac (SCDTL) and a 65-200 MeV, variable energy 2998 MHz Side Coupled Linac (SCL). The status of the project will be presented. The 7 MeV injector is installed at ENEA-Frascati laboratories. The first SCDTL module structure, composed by nine DTL tanks coupled by eight side cavities, has been built and tested on RF bench, so that it is ready for proton acceleration. The results of the measurements done will be also shown.

  17. Status of the TOP Linac project

    The TOP Linac (Oncological Therapy with Protons), under development by ENEA and ISS is a sequence of three pulsed (5 μs 300 Hz) linear accelerators: a 7 MeV, 425 MHz RFQ+DTL (AccSys Model PL-7), a 7-65 MeV, 2998 MHz Side Coupled Drift Tube Linac (SCDTL) and a 65-200 MeV, variable energy 2998 MHz Side Coupled Linac (SCL). The status of the project will be presented. The 7 MeV injector is installed at ENEA-Frascati laboratories. The first SCDTL module structure, composed by nine DTL tanks coupled by eight side cavities, has been built and tested on RF bench, so that it is ready for proton acceleration. The results of the measurements done will be also shown

  18. LINAC4 low energy beam measurements

    Hein, L M; Lallement, J B; Lombardi, A M; Midttun, O; Posocco, P; Scrivens, R

    2012-01-01

    Linac4 is a 160 MeV normal-conducting linear accelerator for negative Hydrogen ions (H−), which will replace the 50 MeV proton Linac (Linac2) as linear injector for the CERN accelerators. The low energy part, comprising a 45 keV Low Energy Beam Transport system (LEBT), a 3 MeV Radiofrequency Quadrupole (RFQ) and a Medium Energy Beam Transport (MEBT) is being assembled in a dedicated test stand for pre-commissioning with a proton beam. During 2011 extensive measurements were done after the source and after the LEBT with the aim of preparing the RFQ commissioning and validating the simulation tools, indispensable for future source upgrades. The measurements have been thoroughly simulated with a multi-particle code, including 2D magnetic field maps, error studies, steering studies and the generation of beam distribution from measurements. Emittance, acceptance and transmission measurements will be presented and compared to the results of the simulations.

  19. Integrated design of the SSC linac injector

    The Ion Source, Low Energy Beam Transport (LEBT), and Radio Frequency Quadrupole (RFQ) of the Superconducting Super Collider (SSC) Linac act as a unit (referred to as the Linac Injector), the Ion Source and LEBT being cantilevered off of the RFQ. Immediately adjacent to both ends of the RFQ cavity proper are endwall chambers containing beam instrumentation and independently-operated vacuum isolation valves. The Linac Injector delivers 30 mA of H- beam at 2.5 MeV. This paper describes the design constraints imposed on the endwalls, aspects of the integration of the Ion Source and LEBT including attachment to the RFQ, maintainability and interchangeability of LEBTs, vacuum systems for each component, and the design of necessary support structure. (Author) 2 tab

  20. An Object-Oriented linac control system

    The ESRF linac has been working since the start of its commissioning (1991) with an industrial turnkey Control System which was not giving reliable service and was difficult to interface to the ESRF machine control system (MCS). It was decided in 1992 to redesign the entire linac electronic interface, using ESRF standards. Following this, it was decided to redesign the control system and to integrate it as part of the proven ESRF distributed control system [W.D. Klotz, Proc. Int. Conf. on Accelerator and Large Physics Experiments (ICALEPS-91), Tsukuba, Japan]. Preparation of the software began in spring 93. The installation and commissioning of the hardware and software has been carried out during a six week summer shutdown. The linac delivered its first beam on schedule using the complete control software. ((orig.))

  1. Energy Recovery Linacs for Commercial Radioisotope Production

    Sy, Amy [Jefferson Lab, Newport News, VA; Krafft, Geoffrey A. [Jefferson Lab, Newport News, VA; Johnson, Rolland [Muons, Inc., Batavia, IL; Roberts, Tom; Boulware, Chase; Hollister, Jerry

    2015-09-01

    Photonuclear reactions with bremsstrahlung photon beams from electron linacs can generate radioisotopes of critical interest. An SRF Energy Recovery Linac (ERL) provides a path to a more diverse and reliable domestic supply of short-lived, high-value, high-demand isotopes in a more compact footprint and at a lower cost than those produced by conventional reactor or ion accelerator methods. Use of an ERL enables increased energy efficiency of the complex through energy recovery of the waste electron beam, high electron currents for high production yields, and reduced neutron production and shielding activation at beam dump components. Simulation studies using G4Beamline/GEANT4 and MCNP6 through MuSim, as well as other simulation codes, will design an ERL-based isotope production facility utilizing bremsstrahlung photon beams from an electron linac. Balancing the isotope production parameters versus energy recovery requirements will inform a choice of isotope production target for future experiments.

  2. Motion equation of a finite dynamic elastic plane lineal element plane lineal element Ecuación del movimiento de un elemento finito lineal plano elástico dinámico con ocho grados de libertad

    Américo G Hossne

    2010-12-01

    Full Text Available A lineal finite element with constant traverse section, it can adopt any orientation in the plane, and their ends or nodes tie it to the rest of the elements. The kinetic energy (T and potential (V of a dynamic elastic element are the basement in the implementation of the Hamilton principle for the definition of a finite element. The definition of the kinetic energy and potential is the first step for the preliminary variational formulation to the enunciation for finite elements that it is used to solve, say, the problems of mechanisms that move in the plane using the Hamilton equation. The general objective consisted on defining the equation of the movement of a finite lineal dynamic elastic plane element using the equation of Hamilton, starting from the lagrangiana (T − V obtained with the use of a polynomial of fifth and first degree, with eight degrees of freedom, four in each node that represented the deformations: axial (u(x, traverse (w(x, slope ((dw(x/dx and bend ((d2w(x/dx2. The deformation due to traverse shearing, insignificant with respect to flexional and axial deformations, the rotational inertia and the frictional forces in the nodes, were underrated with the purpose of producing a friendly element. The specific objectives were to take place: (a the translational mass matrix [MD], (b the translational gyroscopic matrix [AD], (c the translational total rigidity matrix [KD], and (d the deformation vector (S. As a result the movement equation of a finite lineal dynamic elastic plane element was forged [MD]( ¨ S − 2¨[AD]( ˙S + {[K] − ˙2[MD] − ¨[AD]}(S = (Q . On concluded that the equation obtained variationally with the application of the Hamilton Principle is the state–of–the–art pattern, and that the procedure can be used when it is required to increase the number of the pattern freedom degrees.Un elemento finito lineal con sección transversal constante puede adoptar cualquier orientación en el plano y sus

  3. Development of the High Energy Linac Systems

    The main purpose of this project is studying the extension plan of the proton engineering frontier project (PEFP) 100-MeV Linac. It includes three categories. One is studying operation plan of the PEFP linac and its extended accelerators, and developing a distribution system of 100-MeV proton beams with a laser striping. Other is designing superconducting RF (SRF) modules and fabricating and testing a copper cavity model. The other is designing a rapid cycling synchrotron (RCS). The operation scheme of the PEFP linac is related to the optimization in the operation of the 100-MeV linac, 200-MeV SRF, and RCS. We studied several operational method to increase the validity of the accelerators. The beam distribution system has two roles. One is supplying proton beams of 100 MeV to the user group. The laser stripping of the negative hydrogen atoms is used in this case. The other beams are directed to the next high energy accelerators. This study contributes to increase the availability of the proton beams. The SRF is one of candidates to extend the PEFP linac system. Since the accelerating gradient of the SRF is much higher than the normal conducting accelerator, a lot of institutes over the world are developing the SRF structure. Main purposes are designing an SRF module, fabricating and testing an copper model which has similar material properties as Nb of the usual SRF cavity material. The RCS is a synchrotron whose injector is the PEFP 100-MeV linac. Main purposes are determining the lattice structure, studying the fast and slow extraction system, simulating beam behavior in the designed synchrotron. The RCS will be used as the spallation neutron source and tools in the basic and applied science including medical application

  4. Development of the Medium Energy Linac Systems

    The main purpose of this project is developing 100-MeV proton linear accelerator (linac) for proton engineering frontier project (PEFP). In the first phase of the PEFP, the development of the 20-MeV linac has successfully finished. Hence the work scope of this project is designing the linac to accelerate proton beams from 20-MeV up to 100-MeV, fabricating the linac up to 45 MeV, fabricating one set of the medium energy beam transport (MEBT) tank, and developing the low level radio frequency (LLRF) system and the control system. The basic role of the new proton accelerator is accelerating 20-mA proton beams from 20 MeV up to 100 MeV. The first step of the design procedure is optimizing and determining the accelerator parameters. The beam loss is also main concern in the design stage. The drift tube (DT) and the quadrupole magnets are designed to be optimized to the new linac design. The other purpose is confirming the new design by fabricating and tuning the drift tube linac (DTL). The 20MeV proton beam divided into two directions. One is supplying the beams to user group by turning on the 45-degree bending magnet. The other is guided into the 100-MeV DTL by tuning off the dipole magnet. That is why the PEFP MEBT located after 20-MeV DTL. The MEBT is realized as two small DTL tanks with three cells and a 45-degree bending magnet. The fabrication of one MEBT tank is another purpose of this project. The other purposes of this project is developing the LLRF system to control the RF signal and control system to monitor and control the vacuum system, magnet power supply, etc

  5. Beam lines from Linac 1 and Linac 2 to the Booster

    1978-01-01

    View against the direction of the beams. Both Linacs are behind the concrete wall at the back of the picture. The 50 MeV proton beam from Linac 1 enters the PS tunnel through the hole at left. The line from Linac 2, in the process of being installed, comes from the hole at right. The lines converge at a switching magnet (prominently in the foreground), which selects which of the 2 beams to send on to the Booster. See also 7802261 and further explanations there.

  6. Preinjector for Linac 1, accelerating column

    1974-01-01

    For a description of the Linac 1 preinjector, please see first 7403070X. High up on the wall of the Faraday cage (7403073X) is this drum-shaped container of the ion source (7403083X). It is mounted at the HV end of the accelerating column through which the ions (usually protons; many other types of ions in the course of its long history) proceed through the Faraday cage wall to the low-energy end (at ground potential) of Linac 1. The 520 kV accelerating voltage was supplied by a SAMES generator (7403074X).

  7. Linac design algorithm with symmetric segments

    The cell lengths in linacs of traditional design are typically graded as a function of particle velocity. By making groups of cells and individual cells symmetric in both the CCDTL AND CCL, the cavity design as well as mechanical design and fabrication is simplified without compromising the performance. We have implemented a design algorithm in the PARMILA code in which cells and multi-cavity segments are made symmetric, significantly reducing the number of unique components. Using the symmetric algorithm, a sample linac design was generated and its performance compared with a similar one of conventional design

  8. 4-rod RFQ linac for ion implantation

    Fujisawa, Hiroshi; Hamamoto, Nariaki; Inouchi, Yutaka [Nisshin Electric Co. Ltd., Kyoto (Japan)

    1997-03-01

    A 34 MHz 4-rod RFQ linac system has been upgraded in both its rf power efficiency and beam intensity. The linac is able to accelerate in cw operation 0.83 mA of a B{sup +} ion beam from 0.03 to 0.91 MeV with transmission of 61 %. The rf power fed to the RFQ is 29 kW. The unloaded Q-value of the RFQ has been improved approximately 61 % to 5400 by copper-plating stainless steel cooling pipes in the RFQ cavity. (author)

  9. Error analysis in post linac to driver linac transport beam line of RAON

    Kim, Chanmi; Kim, Eun-San

    2016-07-01

    We investigated the effects of magnet errors in the beam transport line connecting the post linac to the driver linac (P2DT) in the Rare Isotope Accelerator in Korea (RAON). The P2DT beam line is bent by 180-degree to send the radioactive Isotope Separation On-line (ISOL) beams accelerated in Linac-3 to Linac-2. This beam line transports beams with multi-charge state 132Sn45,46,47. The P2DT beam line includes 42 quadrupole, 4 dipole and 10 sextupole magnets. We evaluate the effects of errors on the trajectory of the beam by using the TRACK code, which includes the translational and the rotational errors of the quadrupole, dipole and sextupole magnets in the beam line. The purpose of this error analysis is to reduce the rate of beam loss in the P2DT beam line. The distorted beam trajectories can be corrected by using six correctors and seven monitors.

  10. Neutron and photon spectra in LINACs

    A Monte Carlo calculation, using the MCNPX code, was carried out in order to estimate the photon and neutron spectra in two locations of two linacs operating at 15 and 18 MV. Detailed models of both linac heads were used in the calculations. Spectra were estimated below the flattening filter and at the isocenter. Neutron spectra show two components due to evaporation and knock-on neutrons. Lethargy spectra under the filter were compared to the spectra calculated from the function quoted by Tosi et al. that describes reasonably well neutron spectra beyond 1 MeV, though tends to underestimate the energy region between 10–6 and 1 MeV. Neutron and the Bremsstrahlung spectra show the same features regardless of the linac voltage. - Highlights: ► With MCNPX code realistic models of two LINACs were built. ► Photon and neutron spectra below the flattening filter and at the isocenter were calculated. ► Neutron spectrum at the flattening filter was compared against the Tosi et al. source-term model. ► Tosi et al. model underestimates the neutron contribution below 1 MeV. ► Photon spectra look alike to those published in literature.

  11. Induced radioisotopes in a linac treatment hall

    When linacs operate above 8 MV an undesirable neutron field is produced whose spectrum has three main components: the direct spectrum due to those neutrons leaking out from the linac head, the scattered spectrum due to neutrons produced in the head that collides with the nuclei in the head losing energy and the third spectrum due to room-return effect. The third category of spectrum has mainly epithermal and thermal neutrons being constant at any location in the treatment hall. These neutrons induce activation in the linac components, the concrete walls and in the patient body. Here the induced radioisotopes have been identified in concrete samples located in the hall and in one of the wedges. The identification has been carried out using a gamma-ray spectrometer. - Highlights: • Portland cement samples were located inside a treatment hall with a 15 MV linac. • Induced radioisotopes were measured with a NaI(Tl) γ-ray spectrometer. • 56Mn, 24Na, and 28Al were identified and the specific activity was estimated. • In a wedge, 56Mn was induced by the photoneutrons

  12. Upgrade of GUI for linac control

    We are now upgrading GUI(Graphical User Interface) of the control system at Tohoku Linac. This system uses Personal Computer (DECpc466D2LP-66MHz) and Visual Basic which makes coding GUI easy and simple. The first results of this system are presented. (author)

  13. Status of the Novosibirsk energy recovery linac

    The Novosibirsk terahertz free electron laser is based on the energy recovery linac (ERL) with room-temperature radiofrequency system. Some features of the ERL are discussed. The results of emittance measurements and electron optics tests are presented. The second stage of the ERL, which has four orbits, is described briefly

  14. Linac based radiosurgery and stereotactic radiotherapy

    The following topics were discussed: Definition of stereotactic radiosurgery (SRS) and stereotactic radiotherapy (SRT); Stereo market; Indications for SRS/SRT; History of linac-based SRS/SRT; Variety of systems; QA for SRS; Localization; and Imaging. (P.A.)

  15. First beam in Linac4 DTL

    Katarina Anthony

    2014-01-01

    Following the installation of the Linac4 Drift Tube Linac (DTL) earlier this summer (see here), the first DTL tank saw beams at 12 MeV on 5 August.   Transverse emittance measured at 12 MeV after the DTL tank1 using a temporary slit-and-grid emittance device. You never forget your first beam. That was especially true for the Linac4 DTL team, as it followed years of design, construction and vigorous testing. "We performed countless measurements of the geometry, vacuum and magnet polarisation of the DTL tanks while we were in the workshop," says Suitbert Ramberger, project engineer for the Linac4 DTL. "Add that preparation to the excellent RF conditioning that we carried out in the weeks before the beam tests and I was confident that the acceleration with beam would fully meet expectations!" Indeed it did. Beam commissioning tests ran until 21 August and found the DTL operating with nominal transmission. This successful run has confirmed the innovative design ...

  16. Vacuum system for superconducting LINAC at TIFR

    The superconducting heavy ion LINAC booster at the TIFR-BARC facility has been operational. Seven super conducting cryostats containing 4 quarter wave resonators each along with beam lines, bending magnets, switching magnet, diagnostics and vacuum system have been commissioned. The heart of the cryogenic system for the heavy ion superconducting LINAC booster is a custom-built liquid helium refrigerator made by Linde Kryotechnik, Switzerland. The Refrigerator is rated for 300 Watts at 4.5 K with a dual JT (Joule-Thomson valve) at the final cooling stage, which allows simultaneous connections to the cryogenic loads (the LINAC module cryostats) and to a liquid helium storage dewar (1000 litres). The two-phase helium at 4.5 K produced at the JT stage in the refrigerator is delivered to the cryostats through a cryogenic distribution system. The cryogenic distribution system for the LINAC is designed to deliver both liquid helium and liquid nitrogen to the cryostats. The details of UHV system, indigenously developed beam line components, pumps and module cryostats will be presented

  17. Preinjector for Linac 1, ion source

    1974-01-01

    For a description of the Linac 1 preinjector, please see first 7403070X. Inside the drum-shaped container shown in 7403081X, is the ion source with its associated electronics. It sits at the HV end of the accelerating column seen also in 7403081.

  18. Making electron beams for the SLC linac

    A source of high-intensity, single-bunch electron beams has been developed at SLAC for the SLC. The properties of these beams have been studied extensively utilizing the first 100-m of the SLAC linac and the computer-based control system being developed for the SLC. The source is described and the properties of the beams are summarized. (orig.)

  19. Linac LU-20 as injector of Nuclotron

    The linac LU-20 created as an injector of Synchrophasotron and Nuclotron is described. Tables of main parameters and beam intensities are included. The functional diagram of LU-20 is shown. Injection channels, diagnostic and control systems are described also. The scheme of beam transport line is also provided. (author)

  20. Operating experience of 10 MeV industrial linac

    For the past three years, an Industrial 10 MeV RF Electron linac has been in operation at Electron Beam Centre, Navi Mumbai. This pulsed linac has an on-axis coupled cavity bi-periodic π/2 structure and operates at frequency of 2856 MHz. The linac has been tested up to a maximum beam power of 5 kW and is being used for industrial applications. A successful 24-hour continuous run, at 3 kW, established the long term stability of all the linac parameters. This paper describes the high power operating experience of the 10 MeV linac. Details of RF conditioning and performance of the linac during long term tests is presented. Effect of various linac parameters, including injection voltage, RF input power, PRF, gun filament heating power, on the output beam power and energy has been discussed. (author)

  1. Estudio de procesos y herramientas aplicables a la generalización vectorial de entidades lineales.

    Arranz Justel, José Juan; Novoa Plasencia, Andrés; Sánchez Tamargo, David

    2010-01-01

    Se presenta un estudio de algoritmos que ofrecen resultados óptimos en cuanto a lo que a la generalización vectorial de entidades lineales se refiere. Este estudio se encuentra dentro del marco del proyecto CENIT España Virtual para la investigación de nuevos algoritmos de procesado cartográfico. La generalización constituye uno de los procesos cartográficos más complejos, cobrando su mayor importancia a la hora de confeccionar mapas derivados a partir de otros a mayores escalas. ...

  2. GPCs en espacio de estados para el control de sistemas no lineales.

    Salcedo Romero de Ávila, José Vicente

    2008-01-01

    En esta tesis doctoral se aborda el control de sistemas no lineales mediante el empleo de controladores predictivos generalizados (GPCs) en espacio de estados. En primer lugar se realiza una revisión de la metodología de diseño del GPC en la versión entrada/salida (E/S). Partiendo de esta revisión se propone un modelo CARIMA en espacio de estados para el GPC que permite diseñar al mismo utilizando una menor cantidad de memoria y un menor tiempo de cómputo, así como de reducir la complejidad a...

  3. Métodos iterativos para la solución de un sistema de ecuaciones lineales

    Díaz, Julio C.

    2013-01-01

    En este artículo se presenta una introducción a los Métodos Iterativos para la solución de Sistemas de Ecuaciones Lineales. Se da la descripción de los métodos de Gauss-Seidel, Jacobi y S.O.R. Se prueba la convergencia de los métodos asumiendo ciertas propiedades de los sistemas. Se comparan los distintos métodos en su eficiencia y en su utilización de memoria.

  4. Las situaciones problema mediadoras de aprendizajes significativos de la ecuación lineal

    Guerra Valladales, Falner de Fredy

    2014-01-01

    Resumen: El aprendizaje de las ecuaciones lineales es fundamental para el estudio del álgebra, su enseñanza en la secundaria se ha enfocado principalmente en la aplicación de algoritmos, esta forma de enseñanza lleva a que gran parte de los estudiantes no las comprendan y es una práctica que en muchos casos termina siendo un ejercicio de aprendizaje memorístico que luego es olvidado por la mayoría. Esta problemática no es ajena a los estudiantes de secundaria de la Institución Educativa Ciuda...

  5. Desarrollo de la habilidad algoritmizar en el álgebra lineal

    Vargas, Anelys; Blanco, Ramón; Pérez, Olga; Rodríguez, Elizabeth

    2013-01-01

    El presente trabajo tiene como objetivo poner a consideración la propuesta de un proyecto de investigación sobre el desarrollo de habilidades matemáticas en la carrera Ingeniería en Ciencias Informáticas, específicamente, ¿cómo contribuir desde el Álgebra Lineal al desarrollo de la habilidad algoritmizar? Esta es una de las habilidades básicas a desarrollar en los estudiantes de las carreras de perfil computacional e informático, ya que deberán ser utilizadas por ellos en disciplinas propias ...

  6. Los Documentos en lineal B de Micenas ensayo de interpretación global /

    Varias García, Carlos

    2008-01-01

    Un estudio de las 65 tablillas y 8 nódulos de arcilla en lineal b procedentes de Micenas (Grecia), datados entre 1250 y 1200 a.c., a partir de la última edición de los textos: -Olivier, J.-P. y Melena, J.L., Tithemy, Salamanca 1991, intenta esclarecer el funcionamiento del palacio de Micenas en el siglo XIII a.c. El estudio combina los análisis arqueológico y filológico. Los cuatro primeros capítulos analizan los cuatro establecimientos palaciegos en donde se han hallado el grueso de los text...

  7. Comunicación y control de un sistema de desplazamiento lineal para robots manipuladores

    López Sanz, Jose María

    2015-01-01

    Los robots industriales manipuladores son una herramienta imprescindible en la industria del sigo XXI, así como los sistemas para dotar de capacidad de desplazamiento a dichos robots. En este proyecto se profundiza en la comunicación y control de uno de estos sistemas de desplazamiento lineal de alta precisión. En la primera parte del proyecto se diseña la comunicación entre la unidad de control del sistema y un ordenador mediante el protocolo SoE, que es una implementación de ...

  8. Subsistemas singulares de un sistema lineal. Una aproximación a los subespacios cuasiinvariantes

    Puerta Coll, Xavier

    2007-01-01

    Dado un sistema lineal ˙x = Ax + By, se definen los subespacios cuasi-(A, B)- invariantes como aquellos tales que para cada condición inicial en el subespacio, existe un control u(t) que hace que la correspondiente trayectoria, pertenezca enteramente en un entorno arbitrariamente próximo al subespacio. En este trabajo caracterizamos los subespacios cuasi-(A, B)-invariantes a través de existencia de un sistema singular, que puede interpretarse como la restricción del sistema definido por (A, B...

  9. Alfabeto lineal y cuneiforme: relaciones en el II Milenio A.C.

    Vita, Juan-Pablo

    2004-01-01

    La historia del sistema alfabético de escritura en el antiguo Oriente Próximo sigue siendo un campo de investigación fecundo. A pesar de importantes estudios recientes consagrados al tema, son diversas las cuestiones que merecen un estudio más detenido. El sistema alfabético empleó en el II milenio a.C., especialmente en su segunda mitad, dos tipos principales de escritura; el lineal (alfabeto de tipo fenicio) y el cuneiforme(alfabeto de tipo ugarítico). El trabajo que presentamos analiza las...

  10. Photons and photoneutrons spectra of a Linac of 15 MV; Espectros de fotones y fotoneutrones de un LINAC de 15 MV

    Benites R, J. L.; Carrillo C, A. [Centro Estatal de Cancerologia de Nayarit, Av. Enfermeria, Fracc. Fray Junipero Serra, 63000 Tepic, Nayarit (Mexico); Vega C, H. R. [Universidad Autonoma de Zacatecas, Unidad Academica de Estudios Nucleares, Calle Cipres No. 10, Fracc. La Penuela, 98068 Zacatecas (Mexico); Velazquez F, J. B., E-mail: jlbenitesr@prodigy.net.mx [Universidad Autonoma de Nayarit, Posgrado CBAP, Carretera Tepic Compostela Km. 9, Xalisco, Nayarit (Mexico)

    2011-10-15

    Using the Monte Carlo code MCNP-5, the photons and photoneutrons spectra generated in the head stock of the lineal accelerator (Linac) Varian of 15 MV of the Cancerology State of Nayarit were determined. For the calculations a heterogeneous head stock was modeled, more compatible with the work conditions. In the center of the head stock a tungsten target was located on a copper support, followed by the flattened filter. The photons and photoneutrons spectra were obtained accelerating electrons and making them collide against the target to produce photons by Bremsstrahlung, these photons were transported inside the head stock and the photons and photoneutrons spectra were calculated in a punctual detector located under the flattened filter and in the isocenter. The spectra were evaluated in punctual detectors that were located in the plane from the isocenter to the long of the X and Y axes each 20 cm, in an equidistant way, up to 2 m, so much in the longitudinal and transversal axes. In the calculations were used histories 5E(6) with the purpose of obtaining smaller uncertainties to 1%. It was found that the photons spectrum in the punctual detector inside the head stock presents a pick of 1.25 MeV in the energy interval of 0.5 and 1.5 MeV, later suffers a filtration and diminishes in asymptote form. This spectrum modifies when the beam reaches the isocenter, diminishing the low energy photons. Inside the head stock the photoneutrons spectrum shows a structure with two picks, one before 1 MeV and other after 1 MeV; this is for effect of the collimators geometry and the distance. Finally an increment of the total neutrons flow to 60 cm of distance of the isocenter on the Y axis was observed, due to the design geometry of the modeling heterogeneous head stock. (Author)

  11. Comportamiento viscoelástico lineal de soluciones acuosas de ctab/nasal

    Jesús Ramiro Aragón Guajardo

    2015-05-01

    Full Text Available En este trabajo se lleva a cabo un estudio de los comportamientos viscoelásticos lineales de disoluciones acuosas de Bromuro de Cetiltrimetilamonio (CTAB/Salicilato de Sodio (NaSal variándose tanto la temperatura como la concentración de NaSal. La concentración de CTAB se mantuvo constante en 100 mM, mientras que la concentración de NaSal se varió en el intervalo de 35 a 500 mM a las temperaturas de medición de 25, 30 y 35ºC. Los resultados de viscosidad estática indican que el sistema exhibe cuatro regiones con igual número de transiciones estructurales de micelas alargadas filiformes en función de la concentración de NaSal y de la temperatura. Los análisis viscoelásticos fueron llevados a cabo utilizando los modelos mecánicos de Maxwell y Hess, permitiendo obtener una correlación entre la viscoelasticidad lineal oscilatoria, por medio de los espectros de tiempos de relajación, y las diferentes estructuras micelares de cada una de las diferentes regiones del diagrama fisicoquímico dinámico.

  12. Application of the non lineal dynamics to the design of processes in the administration of quality

    The design of processes is a fundamental pillar inside a System of Total Administration of Quality. The great majority of the problems that you/they happen in an organization - 85% - they are caused by the processes, not for the employees. When the processes are not well designed the problems arise: errors, waste, losses of time, delays, duplication take place of the work, flaws of teams and in the worst cases, the client's dissatisfaction. This influences negatively in the Costs of Non conformity. In the work he/she thinks about the possibility to apply the techniques from the non lineal dynamics to the one design of processes like a complex but realer tool that the statistical techniques. As study object the process of production of lead containers is used (means of shielding) that are used to carry radioisotopes in the System of Health of Cuba. He/she intends a model of non lineal dynamics of the process that allows to evaluate what so predictable it is the chosen system (entrance Control to the matter prevails) and which the one will be behavior average of the same one based in the complex interactions that arise in the relationships client-supplier, operative-machine, supplier-supplier, operative-environment and operative-method. Each one of these interactions constitutes a source of uncertainty in the one. I process and he/she has a weight on the temporary dynamics of the characteristic of real quality (homogeneity of the shielding) in the process

  13. Measurements of lineal energy spectra for the BNCT test beam of THOR

    A 2.5 cm tissue-equivalent Rossi type proportional counter was fabricated at St Andrews University and used in this study. Boron-doped and non-boron chambers were performed to measure the lineal energy spectra of a test epithermal neutron beam, built for the research of boron neutron capture therapy (BNCT) at Tsing Hua Open-pool Reactor (THOR). Measurements were made using standard microdosimetry equipment, including a low pressure gas flow system, low noise charge sensitive preamplifier, linear amplifier, multi-channel analyzer, and americium-241 calibration alpha source. Chambers were positioned at different depths in an acrylic phantom. Lineal energy spectra were determined for several gas pressures to simulate various cell sizes. Spectra of the boron-doped chamber are dominated by a peak at ∼200 keV/μm corresponding to the traversal of alpha particles and lithium recoils through the chamber. Peaks in the non-boron spectra correspond to gamma-rays, recoil protons, and fast neutrons. (author)

  14. Re-circulating linac vacuum system

    The vacuum system for a proposed 2.5 GeV, 10ΜA recirculating linac synchrotron light source [1] is readily achievable with conventional vacuum hardware and established fabrication processes. Some of the difficult technical challenges associated with synchrotron light source storage rings are sidestepped by the relatively low beam current and short beam lifetime requirements of a re-circulating linac. This minimal lifetime requirement leads directly to relatively high limits on the background gas pressure through much of the facility. The 10ΜA average beam current produces very little synchrotron radiation induced gas desorption and thus the need for an ante-chamber in the vacuum chamber is eliminated. In the arc bend magnets, and the insertion devices, the vacuum chamber dimensions can be selected to balance the coherent synchrotron radiation and resistive wall wakefield effects, while maintaining the modest limits on the gas pressure and minimal outgassing

  15. Bunch Shape Monitor for SSCL linac

    The Superconducting Super Collider Laboratory and the Institute for Nuclear Research ore collaboratively developing a Bunch Shape Monitor diagnostics for commission the SSCL linac. The Bunch Shape Monitor is designed to measure the intensity of beam as a function of time over the micro-bunch of the beam. Design resolution for the SSCL monitors is approximately 7 psec. The first monitor will operate at the fundamental frequency of 428 MHz and will be used to measure the output beam of the RFQ Linac. First available results will be presented and compared with predictions. Further development will allow the monitors to fit in a standard SSCL beam box and one will operate at the third harmonic of 428 MHz. Proposals to use the Bunch Shape Monitor to measure the longitudinal phase space distribution of the beam will be discussed

  16. Bunch shape measurements at the INR linac

    The bunch shape analyser (BSA) has been developed in the INR and is used for the INR linac tuning. The operation of the device is based on a transverse scanning of a low energy secondary electrons emitted from a thin target crossed by an accelerated beam. The phase resolution obtained is better than 1deg (f = 198.2 MHz). The results of the bunch shape measurements at the exit of the first (20 MeV) accelerating cavity as well as at the exit of the drift tube linac part (100 MeV) of the accelerator are presented. The methods and the results of rf amplitudes and phases setting and a longitudinal emittance measurements with the help of BSA are described. (author)

  17. Bunch shape monitor for SSCL linac

    The Superconducting Super Collider Laboratory and the Institute for Nuclear Research are collaboratively developing a Bunch Shape Monitor diagnostic for commissioning the SSCL linac. The Bunch Shape Monitor is designed to measure the intensity of beam as a function of time over the micro-bunch of the beam. Design resolution for the SSCL monitors is approximately 7 psec. The first monitor will operate at the fundamental frequency of 428 MHz and will be used to measure and output beam of the RFQ Linac. First available results will be presented and compared with predictions. Further development will allow the monitors to fit in a standard SSCL beam box and one will operate at the third harmonic of 428 MHz. Proposals to use the Bunch Shape Monitor to measure the longitudinal phase space distribution of the beam will be discussed

  18. Electronics Platform of PS Linac 1 Preinjector

    1974-01-01

    For servicing during shutdowns, a draw-bridge from a door in the Faraday cage led to the "electronics platform" of the linac 1 preinjector (at 520 kV when in operation) and the top of the electronics platform was lifted on hydraulic jacks for easy access. Henry Charmot is busy with a service. The platform contained the electronics for the ion source, controlled from outside the Faraday cage via an infrared optical link. The ion source, also at 520 kV potential, is housed in the drum, visible in the background, on the insulator column, which at its right end is mounted at ground potential. Behind the wall, to the right, is the 50 MeV linac 1. See also 7403064X, 7403066X, 7403124.

  19. Simulations for CLIC Drive Beam Linac

    Aksoy, Avni

    2012-01-01

    The Drive Beam Linac of the Compact Linear Collider (CLIC) has to accelerate an electron beam with 4.2 A up to 2.4 GeV in almost fully-loaded structures. The pulse contains about 70000 bunches, one in every second rf bucket, and has a length of 140 $\\mu$s. The beam stability along the beamline is of concern for such a high current and pulse length. We present different options for the lattice of the linac based on FODO, triplet and doublet cells and compare the transverse instability for each lattice including the effects of beam jitter, alignment and beam-based correction. Additionally longitudinal stability is discussed for different bunch compressors using FODO type of lattice.

  20. Induction linacs for heavy ion fusion research

    The new features of employing an induction linac as a driver for inertial fusion involve (1) transport of high-current low-emittance heavy ion beams, (2) multiple independently-focussed beams threading the same accelerator structure, and (3) synthesis of voltage waveforms to accomplish beam current amplification. A research program is underway at LBL to develop accelerators that test all these features with the final goal of producing an ion beam capable of heating matter to approx. 70 eV. This paper presents a discussion of some properties of induction linacs and how they may be used for HIF research. Physics designs of the High Temperature Experiment (HTE) and the Multiple Beam Experiment (MBE) accelerators are presented along with initial concepts of the MBE induction units

  1. Operation of the tandem-linac accelerator

    The tandem-linac accelerator system is operated as a source of energetic heavy-ion projectiles for research in several areas of nuclear physics and occasionally in other areas of science. The accelerator system consists of a 9-MV tandem electrostatic accelerator and a superconducting-linac energy booster that can provide an additional 20 MV of acceleration. A figure shows the layout of this system, which will be operated in its present form until September 1985, when it will be incorporated into the larger ATLAS system. In both the present and future forms the accelerator is designed to provide the exceptional beam quality and overall versatility required for precision nuclear-structure research

  2. Induction linacs for heavy ion fusion research

    Fessenden, T.J.

    1984-05-01

    The new features of employing an induction linac as a driver for inertial fusion involve (1) transport of high-current low-emittance heavy ion beams, (2) multiple independently-focussed beams threading the same accelerator structure, and (3) synthesis of voltage waveforms to accomplish beam current amplification. A research program is underway at LBL to develop accelerators that test all these features with the final goal of producing an ion beam capable of heating matter to approx. 70 eV. This paper presents a discussion of some properties of induction linacs and how they may be used for HIF research. Physics designs of the High Temperature Experiment (HTE) and the Multiple Beam Experiment (MBE) accelerators are presented along with initial concepts of the MBE induction units.

  3. Stereotactic linac radiosurgery for arteriovenous malformations.

    Kenny, B G; Hitchcock, E. R.; Kitchen, G.; Dalton, A E; Yates, D A; Chavda, S V

    1992-01-01

    Stereotactic linear accelerator (linac) radiosurgery has been in operation in the West Midlands since 1987, the first of its kind in the United Kingdom. Forty two patients with high-flow cerebral arteriovenous malformations have been treated, 26 of whom have been followed up. Angiography one year after treatment showed that five lesions were obliterated, 11 were reduced in size and/or flow rate and 10 were unchanged. Overall results show that nine out of 10 patients reviewed at 24 months had ...

  4. Impedances for electron linacs and storage rings

    Some basic concepts and results are presented concerning the impedances of electron linacs and storage rings. The impedances of an accelerator or ring completely characterizes the interaction of the beam with its environment. Not only does the impedance (or its Fourier transform, the wake potential) determine the energy loss by a bunched beam to its environment, but it is also the chief ingredient required for any calculation of beam stability

  5. Making electron beams for the SLC linac

    A source of high-intensity, single-bunch electron beams has been developed at SLAC for the SLC. The properties of these beams have been studied extensively utilizing the first 100-m of the SLAC linac and the computer-based control system being developed for the SLC. The source is described and the properties of the beams are summarized. 9 references, 2 figures, 1 table

  6. Injection schemes for the TOP Linac

    In this report two schemes are studied for the injection in the SCDTL section of the TOP Linac of the proton beam produced by a 7 MeV linear accelerator. The project derives by an agreement between ENEA (National Agency for New Technology, Energy and Environment) and ISS. In these new versions of the design the constraint of a synchronization of the radio frequencies of the two accelerators is suppressed

  7. Photocathodes for the energy recovery linacs

    Rao, T.; Burrill, A.; Chang, X. Y.; Smedley, J.; Nishitani, T.; Hernandez Garcia, C.; Poelker, M.; Seddon, E.; Hannon, F. E.; Sinclair, C. K.; Lewellen, J.; Feldman, D.

    2006-02-01

    This paper presents an overview of existing and emerging technologies on electron sources that can service various energy recovering linacs under consideration. Photocathodes that can deliver average currents from 1 mA to 1 A, the pros and cons associated with these cathodes are addressed. Status of emerging technologies such as secondary emitters, cesiated dispenser cathodes, field and photon assisted field emitters and super lattice photocathodes are also reviewed.

  8. PHOTOCATHODES FOR THE ENERGY RECOVERY LINACS

    This paper presents an overview of existing and emerging technologies on electron sources that can service various Energy Recovering Linacs under consideration. Photocathodes that can deliver average currents from 1 mA to 1 A, the pros and cons associated with these cathodes are addressed. Status of emerging technologies such as secondary emitters, cesiated dispenser cathodes, field and photon assisted field emitters and super lattice photocathodes are also reviewed

  9. Cost projection for a superconducting linac structure

    The increase of energy of the present 800 MeV proton linac at LAMPF to 1.6 to 2.2 GeV is of primary importance for the proposed future experimental program of this Laboratory. Layout and cost studies have been performed for (a) normalconducting and (b) superconducting accelerating structures. A more recent cost analysis for a superconducting structure is given in this report. 4 figs., 2 tabs

  10. Linac for the National Synchrotron Light Source

    The nominally 100 MeV electron linear accelerator to be used as an injector for the booster synchrotron of the National Synchrotron Light Source is described. The machine utilizes a combination of Varian and SLAC accelerating guides and is interfaced by means of a microprocessor-based Intel Multibus system, to the Data General central control computer. Provision for emittance and momentum measurement is provided in the transport line between the linac and the booster synchrotron