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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. 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

  3. 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...

  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. 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.

  10. 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

  11. 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.

  12. 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...

  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. 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)

  15. 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.

  16. 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...

  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. 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

  1. 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

  2. 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...

  3. 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...

  4. 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 ...

  5. 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...

  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. 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)

  6. 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.

  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. 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...

  4. 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

  5. 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...

  6. 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

  7. 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)

  8. 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.

  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. 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.

  11. 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

  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. 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...

  15. 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 ...

  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. 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.

  8. 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.

  9. 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

  10. 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.

  11. 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)

  12. 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.

  13. 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)

  14. 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.

  15. 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)

  16. 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)

  17. 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...

  18. 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.

  19. 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.

  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. 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.

  2. 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.

  3. 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...

  4. 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)

  5. 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.

  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. 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 (

  13. 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)

  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. 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)

  1. 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.

  2. 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)

  3. 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.

  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. 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...

  6. 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

  7. 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...

  8. 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...

  9. 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.

  10. 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...

  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. 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.

  14. 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)

  15. 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)

  16. 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.

  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. 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

  1. 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)

  2. 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 ...

  3. 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

  4. 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)

  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 ⋅ 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

  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. 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...

  11. 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.

  12. 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.)

  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. 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

  6. 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

  7. 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.

  8. 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.

  9. 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.

  10. 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.

  11. 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

  12. 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.

  13. 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.

  14. 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

  15. 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.)

  16. 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

  17. 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.))

  18. 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)

  19. 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)

  20. 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

  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. 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)

  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. 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).

  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. 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

  11. 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)

  12. 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

  13. 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.)

  14. 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 ...

  15. 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)

  16. 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.

  17. 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.

  18. 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

  19. 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.)

  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. 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.

  2. 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...

  3. 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. ...

  4. 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...

  5. 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...

  6. 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 ...

  7. 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...

  8. 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...

  9. 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 ...

  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. 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

  12. 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

  13. 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

  14. 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)

  15. 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

  16. 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.

  17. 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.

  18. 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

  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. 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

  1. 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)

  2. 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.

  3. 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

  4. 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

  5. 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

  6. 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 ...

  7. 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

  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. 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

  10. 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

  11. 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.

  12. 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

  13. El vacío entre infraestructuras lineales y ciudad: espacios anómalos como oportunidad para lo colectivo

    Rabazo Martín, Marta

    2013-01-01

    Partiendo del estudio del vacío del muro de Berlín en el Laboratorio de Paisaje como infraestructura lineal y espacio anómalo, se pretende profundizar la investigación de los vacíos generados por las infraestructuras lineales que atraviesan nuestras ciudades, espacios marginales, olvidados o apartados de la trama urbana pero llenos de identidad y significado donde se pueden generar nuevas oportunidades para el espacio público. A través de un estudio de casos se intentará analizar la ...

  14. Predicción de ingresos de causas penales utilizando programación genética lineal

    Garcete Rodríguez, Alberto David; Barán, Benjamín

    2015-01-01

    Este trabajo propone una metodología de predicción de ingresos de causas penales utilizando Programación Genética Lineal (Linear Genetic Programming - LGP). El estudio se realizó en base a datos mensuales recogidos durante siete años (2007 a 2013), en los siete Juzgados Penales de Garantías de Ciudad del Este - Paraguay. La verificación del método propuesto se hizo mediante la comparación del método LGP implementado con modelos estadísticos conocidos como la regresión lineal, promedio móvil, ...

  15. ¿Realmente existe convergencia regional en México? Un modelo de datos-panel TAR no lineal

    Domingo Rodríguez-Benavides; Miguel Ángel Mendoza-González; Francisco Venegas-Martínez

    2016-01-01

    Este trabajo analiza la hipótesis de convergencia regional en México para el periodo 1970-2012 por medio de un modelo de crecimiento no lineal. La metodología empleada combina tres enfoques: el modelo panel autorregresivo de umbral (tar, threshold autorregresive), las pruebas de raíces unitarias en panel y el cálculo de los valores críticos a través de simulación bootstraping. Los resultados empíricos del modelo no lineal aplicado al pib per cápita de distintos grupos de estados de la repúbli...

  16. Control no lineal robusto de una maqueta de helicóptero con rotores de velocidad variable

    R. Rubio, Francisco; Vivas Venegas, Carlos; G. Ortega, Manuel; López-Martínez, Manuel

    2007-01-01

    En este artículo se presenta el diseño de un controlador robusto no lineal para un helicóptero de laboratorio. El equipo se caracteriza por tener los ángulos de ataque de las hélices de los rotores fijos y se controla mediante el cambio de velocidad de los rotores a través de dos motores de accionamiento directo. El sistema resultante es multivariable (de 2 entradas y 4 salidas) altamente no lineal y fuertemente acoplado. La aplicación presentada en este artículo considera el diseño de un sis...

  17. All Digital IQ Servo-System for CERN Linacs

    Rohlev, A; Garoby, R

    2003-01-01

    A new VME based system has been developed and built at CERN for the servo loops regulating the field in the linac accelerating structure. It makes use of high speed digital In-phase/Quadrature (IQ) detection, digital processing, and digital IQ modulation. The digital processing and IQ modulation is done in a single PLD. The system incorporates continually variable set points, iterative learning, feed forward as well as extensive diagnostics and other features well suited for digital implementations. Built on a single VME card, it will be first used in the energy ramping RF chain of the CERN Heavy Ion Linac (linac 3) and later for upgrading the present proton linac (linac 2). This system serves also as a prototype for the future Superconducting Proton Linac (SPL). The design principle and the experimental results are described.

  18. Advanced RF power sources for linacs

    Wilson, P.B.

    1996-10-01

    In order to maintain a reasonable over-all length at high center-of-mass energy, the main linac of an electron-positron linear collider must operate at a high accelerating gradient. For copper (non-superconducting) accelerator structures, this implies a high peak power per unit length and a high peak power per RF source, assuming a limited number of discrete sources are used. To provide this power, a number of devices are currently under active development or conceptual consideration: conventional klystrons with multi-cavity output structures, gyroklystrons, magnicons, sheet-beam klystrons, multiple-beam klystrons and amplifiers based on the FEL principle. To enhance the peak power produced by an rf source, the SLED rf pulse compression scheme is currently in use on existing linacs, and new compression methods that produce a flatter output pulse are being considered for future linear colliders. This paper covers the present status and future outlook for the more important rf power sources and pulse compression systems. It should be noted that high gradient electron linacs have applications in addition to high-energy linear colliders; they can, for example, serve as compact injectors for FEL`s and storage rings.

  19. Wake Field Effect Analysis in APT Linac

    Kurennoy, S 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 (<1 nA/m), that requires analyzing carefully all possible loss sources. While wake-field effects are usually considered negligible in proton linacs, we study these effects for the APT to exclude potential problems at such a high current. Loss factors and resonance frequency spectra of various discontinuities of the vacuum chamber are investigated, both analytically and using 2-D and 3-D simulation codes with a single bunch as well as with many bunches. Our main conclusion is that the only noticeable effect is the HOM heating of the 5-cell SC cavities. It, however, has an acceptable level and, in addition, will be taken care of by HOM couplers.

  20. LINAC4 takes a tour of Europe

    Katarina Anthony

    2011-01-01

    Along the German Autobahnen, a truck carrying 20 tonnes of copper is on its way to Poland. The metal has already made a short tour of Europe, yet the drive across the high-speed highway is only the beginning of its transformation into CERN’s next linear accelerator, LINAC4.   Grzegorz Wrochna (left), director of the Andrzej Soltan Institute for Nuclear Studies (IPJ), and Rolf Heuer (right), CERN DG, sign the framework agreement between the two institutes. By the summer of 2012, the PI-Mode Structures (PIMS) will be constructed and completely installed in the LINAC4 tunnel. The PIMS cavities are the final accelerating structures needed for LINAC4, and have been designed to accelerate protons from 100 to 160MeV. While the first cavity was built entirely at CERN, construction of the remaining cavities has become a larger, multi-national operation. In a 1 million euro framework agreement signed on 11 February by the Director-General, the Andrzej Soltan Institute for Nuclear Studies in Swie...

  1. Machining of cavities for travelling wave LINAC

    A Traveling Wave (T.W.), 2π/3 mode electron linear accelerator of 2856 MHz is under development at CAT for radiation processing of agricultural products. This LINAC consists of a thermionic triode electron gun, TW buncher section and Regular Section. Machining of input/output couplers, regular section cells and disc were carried out using CNC lathe LAL- 2 BT and CNC milling machine BMV - 40. This paper highlights the dimensional and geometrical requirements of cavities, problems encountered during machining of OFE copper and their solutions to achieve high precision with ultrahigh surface finish. The performance of Linac depends upon a number of factors such as operating vacuum level, accuracies of cavity dimensions, materials, and surface finish of cavities comprising the LINAC. Each of these depends upon material and fabrication techniques used for manufacturing OFE copper of higher purity has been used since they offer lower surface resistivity and lower power losses. With CNC tuning and milling machines, the high surface finish has been achieved with higher dimensional and geometrical accuracies

  2. Wake fields in SLAC Linac Collimators

    Novokhatski, Alexander [SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States); Stanford Univ., Stanford, CA (United States); Decker, F. -J. [SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States); Stanford Univ., Stanford, CA (United States); Smith, H. [SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States); Stanford Univ., Stanford, CA (United States); Sullivan, M. [SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States); Stanford Univ., Stanford, CA (United States)

    2014-12-02

    When a beam travels near collimator jaws, it gets an energy loss and a transverse kick due to the backreaction of the beam field diffracted from the jaws. The effect becomes very important for an intense short bunch when a tight collimation of the background beam halo is required. In the Linac Coherent Light Source at SLAC a collimation system is used to protect the undulators from radiation due to particles in the beam halo. The halo is most likely formed from gun dark current or dark current in some of the accelerating sections. However, collimators are also responsible for the generation of wake fields. The wake field effect from the collimators not only brings an additional energy jitter and change in the trajectory of the beam, but it also rotates the beam on the phase plane, which consequently leads to a degradation of the performance of the Free Electron Laser at the Linac Coherent Light Source. In this paper, we describe a model of the wake field radiation in the SLAC linac collimators. We use the results of a numerical simulation to illustrate the model. Based on the model, we derive simple formulas for the bunch energy loss and the average kick. In addition, we also present results from experimental measurements that confirm our model.

  3. Preinjector for Linac 1, Faraday cage

    1974-01-01

    The 50 MeV Linac 1 started up in 1958 as injector to the 26 GeV PS, with a 520 kV Cockcroft-Walton generator as its preinjector, housed in a vast Faraday cage, visible here. When the Cockcroft-Walton broke down in 1973, it was replaced by a much smaller SAMES generator, of the kind used for electrostatic separators. From 1980 on, Linac 2 took over as injector for the 800 MeV Booster, and Linac 1 continued as injector for LEAR. In 1984, the electrostatic preinjector (i.e. the Faraday cage with its contents, SAMES generator and all) was replaced by a 520 keV RFQ. At the lower left corner we see the HV connectors to the SAMES generator, at the right edge part of the opened electronics-platform. Jean-Luc Vallet sees to it that all parts are properly grounded. See also 7403073X, 7403074X, 7403081X, 7403083X.

  4. A 2--4 nm Linac Coherent Light Source (LCLS) using the SLAC linac

    We describe the use of the SLAC linac to drive a unique, powerful. short wavelength Linac Coherent Light Source (LCLS). Operating as an FEL, lasing would be achieved in a single pass of a high peak current electron beam through a long undulator by self-amplified spontaneous emission (SASE). The main components are a high-brightness rf photocathode electron gun; pulse compressors; about 1/5 of the SLAC linac; and a long undulator with a FODO quadrupole focussing system. Using electrons below 8 GeV, the system would operate at wavelengths down to about 3 nm, producing ≥10 GW peak power in sub-ps pulses. At a 120 Hz rate the average power is ∼ 1 W

  5. S-band linac-based X-ray source with π/2-mode electron linac

    The activities with the compact X-ray source are attracting more attention, particularly for the applications of the source in medical fields. We propose the fabrication of a compact X-ray source using the SAMEER electron linear accelerator and the KEK laser undulator X-ray source (LUCX) technologies. The linac developed at SAMEER is a standing wave side-coupled S-band linac operating in the π/2 mode. In the proposed system, a photocathode RF gun will inject bunches of electrons in the linac to accelerate and achieve a high-energy, low-emittance beam. This beam will then interact with the laser in the laser cavity to produce X-rays of a type well suited for various applications. The side-coupled structure will make the system more compact, and the π/2 mode of operation will enable a high repetition rate operation, which will help to increase the X-ray yield.

  6. Bunch Extension Monitor for LINAC of SPIRAL2 facility

    Revenko, R.V.; Vignet, J.-L.

    2013-01-01

    Measurements of the bunch longitudinal shape of beam particles are crucial for optimization and control of the LINAC beam parameters and maximization of its integrated luminosity. The non-interceptive bunch extension monitor for LINAC of SPIRAL2 facility is being developed at GANIL. The five bunch extension monitors are to be installed on the entrance of LINAC between superconducting cavities. The principle of monitor operation is based on registration of x-rays induced by ions of accelerator...

  7. Investigations of Slow Motions of the SLAC Linac Tunnel

    Seryi, Andrei

    2000-01-01

    Investigations of slow transverse motion of the linac tunnel of the Stanford Linear Collider have been performed over period of about one month in December 1999 -- January 2000. The linac laser alignment system, equipped with a quadrant photodetector, allowed submicron resolution measurement of the motion of the middle of the linac tunnel with respect to its ends. Measurements revealed two major sources responsible for the observed relative motion. Variation of the external atmospheric pressu...

  8. Review of Linac-Ring Type Collider Proposals

    Akay, A N; Sultansoy, S

    2009-01-01

    There are three possibly types of particle colliders schemes: familiar (well known) ring-ring colliders, less familiar however sufficiently advanced linear colliders and less familiar and less advanced linac-ring type colliders. The aim of this paper is two-fold: to present possibly complete list of papers on linac-ring type collider proposals and to emphasize the role of linac-ring type machines for future HEP research.

  9. Measurements of longitudinal phase space in the SLC linac

    The electron and positron bunch distributions in the Stanford Linear Collider (SLC) linac have been measured using a Hamamatsu, model N3373-02, 500-femtosecond streak camera. The distributions were measured at the end of the SLC linac versus the bunch compressor RF voltage. The energy spread at the end of the linac was also measured using a wire scanner. The effects of the bunch compressor on the shape of the bunch distribution are also presented

  10. Beam position correction in the Fermilab linac

    Orbit correction has long been an essential feature of circular accelerators, storage rings, multipass linacs, and linear colliders. In a drift tube linear accelerator (DTL) such as the H- Linac at Fermilab, beam position monitors (BPMs) and dipole corrector magnets can only be located in between accelerating tanks. Within a tank many drift tubes (from 20 to 60) each house a quadrupole magnet to provide strong transverse focusing of the beam. With good alignment of the drift tubes and quadrupoles and a sufficiently large diameter for the drift tubes, beam position is not typically a major concern. In the Fermilab DTL, 95% of the beam occupies only 35% of the available physical aperture (4.4 cm). The recent upgrade of the Fermilab Linac from a final energy of 200 MeV to 400 MeV has been achieved by replacing four 201.25 MHz drift tube linac tanks with seven 805 MHz side-coupled cavity modules (the high energy portion of the linac or HEL). In order to achieve this increase in energy within the existing enclosure, an accelerating gradient is required that is a factor of 3 larger than that found in the DTL. This in turn required that the physical aperture through which the beam must pass be significantly reduced. In addition, the lattice of the side-coupled structure provides significantly less transverse focusing than the DTL. Therefore in the early portion of the HEL the beam occupies over 95% of the available physical aperture (3.0 cm). In order to prevent beam loss and the creation of excess radiation, the ability to correct beam position throughout the HEL is of importance. An orbit smoothing algorithm commonly used in the correction of closed orbits of circular machines has been implemented to achieve a global least-squares minimization of beam position errors. In order to accommodate several features of this accelerator a refinement in the algorithm has been made to increase its robustness and utilize correctors of varying strengths

  11. Front-end physics design of APT linac

    The accelerator for the Accelerator based Production of Tritium (APT), uses a radio-frequency quadrupole (RFQ), followed by the newly developed coupled-cavity drift tube linac (CCDTL) and a coupled- cavity linac (CCL). The production target requires the APT linac to deliver a 100 mA proton beam with an energy of 1.3 -1.7 GeV. The main challenge in the design comes from the requirement to minimize beam loss. Hands-on maintenance of the entire linac requires very little beam loss

  12. Designs for a Linac-Ring LHeC

    Zimmermann, Frank; /CERN; Bruning, Oliver; /CERN; Ciapala, Edmond; /CERN; Haug, Friedrich; /CERN; Osborne, John; /CERN; Schulte, Daniel; /CERN; Sun, Yipeng; /CERN; Tomas, Rogelio; /CERN; Adolphsen, Chris; /SLAC; Calaga, Rama; /Brookhaven; Litvinenko, Vladimir; /Brookhaven; Chattopadhyay, Swapan; /Cockcroft Inst. Accel. Sci. Tech.; Dainton, John; /Liverpool U.; Klein, Max; /Liverpool U.; Eide, Anders; /Paris U., VI-VII

    2012-06-21

    We consider three scenarios for the recirculating electron linear accelerator (RLA) of a linac-ring type electron-proton collider based on the LHC (LHeC): (i) a pulsed linac with a final beam energy of 60 GeV ['p-60'], (ii) a higher luminosity configuration with two cw linacs and energy-recovery (ERL) also at 60 GeV ['erl'], and (iii) a high energy option using a pulsed linac with 140-GeV final energy ['p-140']. We discuss parameters, synchrotron radiation, footprints, and performance for the three scenarios.

  13. SIMULATIONS OF A MUON LINAC FOR A NEUTRINO FACTORY

    Kevin Beard, Alex Bogacz ,Slawomir Bogacz, Vasiliy Morozov, Yves Roblin

    2011-04-01

    The Neutrino Factory baseline design involves a complex chain of accelerators including a single-pass linac, two recirculating linacs and an FFAG. The first linac follows the capture and bunching section and accelerates the muons from about 244 to 900 MeV. It must accept a high emittance beam about 30 cm wide with a 10% energy spread. This linac uses counterwound, shielded superconducting solenoids and 201 MHz superconducting cavities. Simulations have been carried out using several codes including Zgoubi, OptiM, GPT, Elegant and G4beamline, both to determine the optics and to estimate the radiation loads on the elements due to beam loss and muon decay.

  14. Oxygen ion source and RFQ for Linac 1

    Photographic Service

    1986-01-01

    As injector to the PS Booster, Linac 1 was replaced by Linac 2 in 1980. It continued to be used for the acceleration of oxygen and sulfur ions. In 1984, its Cockcroft-Walton preinjector was replaced by an RFQ. In the foreground at the right is the oxygen ion source. A 90 deg bending magnet selects O6+ ions which are preaccelerated in an RFQ and enter Linac 1, at the far left. In the background is the proton and negative hydrogen ion source, followed by the 520 keV RFQ-1 and a bending magnet towards the entrance of Linac 1.

  15. Boeing 120 MeV RF linac for FEL research

    A new electron linac for high power, visible wavelength, free electron laser research is under construction at the Boeing Radiation Laboratory in Seattle. The linac is a five section, traveling wave, L band structure with a specialized comb pulse format of widely separated high charge micropulses. The paper describes the accelerator design and prototyping of key components of the linac. These include a double subharmonic injector and a long pulse phase and amplitude stabilized RF source which have been tested on Boeing's 20 MeV S band linac

  16. All Digital IQ Servo-System for CERN Linacs

    Broere, J; Garoby, R; Rohlev, A; Serrano, J

    2004-01-01

    A VME based control system has been developed and built at CERN for the servo loops regulating the field in linac accelerating structures. It is an all-digital system built on a single VME card, providing digital detection, processing, and modulation. It is foreseen to be used, in different versions, for the needs of both present and future CERN hadron linacs. The first application will be in the energy ramping RF chain of the CERN Heavy Ion Linac (linac 3). Design principle and the experimental results are described.

  17. Linac4: the final assembly stage is under way

    CERN Bulletin

    2013-01-01

    The Linac4 radiofrequency quadrupole (RFQ) module was installed at the accelerator test-stand in Building 152 last August. After an assembly phase and tests that concluded last March with the acceleration of a hydrogen beam to 3 MeV, the module has just been permanently installed in the new Linac4 tunnel (Building 400). The installation of the MEBT (Medium Energy Beam Transport) will begin shortly, followed by the start of the first Linac4 commissioning phase.     To find out more about the Linac4 RFQ module, read the previous Bulletin articles published in Nos. 21-22/2010 and 35-36/2012.

  18. Effects of Linac Wakefield on CSR Microbunching in the Linac Coherent Light Source

    The design of the Linac Coherent Light Source (LCLS) requires two-stage bunch compression for stability against timing and charge jitters. Coherent synchrotron radiation (CSR) induced in these bunch compressors can drive a microbunching instability that may degrade the beam brightness. In this paper, we study effects of the longitudinal wakefield in the accelerator on this instability. We show that significant energy modulation can be accumulated in the linac through the geometrical wakefield and can enhance the CSR microbunching in these compressors. Analytical calculations are compared with numerical simulations to evaluate the gain of microbunching for the entire LCLS accelerator system.

  19. Effects of Linac Wakefield on CSR Microbunching in the Linac Coherent Light Source

    Huang, Z

    2003-01-01

    The design of the Linac Coherent Light Source (LCLS) requires two-stage bunch compression for stability against timing and charge jitters. Coherent synchrotron radiation (CSR) induced in these bunch compressors can drive a microbunching instability that may degrade the beam brightness. In this paper, we study effects of the longitudinal wakefield in the accelerator on this instability. We show that significant energy modulation can be accumulated in the linac through the geometrical wakefield and can enhance the CSR microbunching in these compressors. Analytical calculations are compared with numerical simulations to evaluate the gain of microbunching for the entire LCLS accelerator system..

  20. Interdigital H -mode drift-tube linac design with alternative phase focusing for muon linac

    Otani, M.; Mibe, T.; Yoshida, M.; Hasegawa, K.; Kondo, Y.; Hayashizaki, N.; Iwashita, Y.; Iwata, Y.; Kitamura, R.; Saito, N.

    2016-04-01

    We have developed an interdigital H-mode (IH) drift-tube linac (DTL) design with an alternative phase focusing (APF) scheme for a muon linac, in order to measure the anomalous magnetic moment and electric dipole moment (EDM) of muons at the Japan Proton Accelerator Research Complex (J-PARC). The IH-DTL accelerates muons from β =v /c =0.08 to 0.28 at an operational frequency of 324 MHz. The output beam emittances are calculated as 0.315 π and 0.195 π mm mrad in the horizontal and vertical directions, respectively, which satisfies the experimental requirement.

  1. First operation of the rf-focused interdigital linac structure

    The new rf-focused interdigital (RFI) linac structure came into operation at the Linac Systems laboratory in May of 2006, after a multi-year development program supported by the US Department of Energy. The RFI linac structure is basically an interdigital (or Wideroee) linac structure with rf quadrupole focusing incorporated into each drift tube. The RFI prototype operates at 200-MHz and consists of an ECR ion source, an Einzel lens LEBT, a radial-strut, four-bar RFQ linac section to 0.75 MeV and an RFI linac section to a final energy of 2.5 MeV. The total length of the prototype is 2.2 m. The RFQ and RFI linac sections are resonantly coupled and require a total of 120 kW of rf power for cavity excitation. The energy of the accelerated beam was confirmed by requiring it to pass through a 2.25-MeV energy-degrading foil. The specifications for the RFI linac prototype were chosen to address the demanding Boron Neutron Capture Therapy medical application. There are, however, many other potential applications for the structure as it has efficiency and size advantages for both protons and heavy ions at a variety of energies and currents. To date, we have achieved a beam current of approximately 1 mA peak at a relatively low duty factor. We continue to improve the performance of the prototype structure on a daily basis as we better understand the optimal operational settings for the prototype system. Now that the first operational milestone for the RFI linac structure has been achieved, Linac Systems will vigorously pursue projects and partnerships for multiple applications such as compact and intense neutron sources, proton and carbon injector linacs for synchrotrons and PET isotope production

  2. Ecuaciones en derivadas parciales con condiciones de contorno no lineales aplicaciones a la dinámica de tumores

    Morales-Rodrigo, Cristian

    2009-01-01

    Esta tesis presenta tres partes: En la primera haremos un estudio teórico general de las ecuaciones elípticas en derivadas parciales con condiciones de contorno no lineales. Posteriormente, en la segunda, haremos un estudio teórico de ecuaciones elíptica

  3. Calculations radiobiological using the quadratic lineal model in the use of the medium dose rate absorbed in brachytherapy. Pt. 3

    Calculations with the quadratic lineal model for medium rate using the equation dose-effect. Several calculations for system of low dose rate brachytherapy plus teletherapy, calculations for brachytherapy with medium dose rate together with teletherapy, dose for fraction and the one numbers of fractions in medium rate

  4. Sobre la existencia y estabilidad de un sistema no-lineal de tipo parabólico

    Bogoya, Mauricio

    2010-01-01

    En este artículo se estudia la existencia y estabilidad de las soluciones de un sistema parabólico no lineal, el cual describe el fenómeno de reacción-difusión de flujo de neutrones en el interior de un reactor de fisión.

  5. Estudio numérico de sistemas de ecuaciones no lineales difusas

    Patricio Cumsille

    2010-01-01

    Full Text Available En este trabajo estudiamos la resolución numérica de sistemas de ecuaciones no lineales difusas. Más precisamente describimos, analizamos y simulamos métodos numéricos, tales como el método de Newton, con el fin de aproximar de forma eficiente las soluciones a dichos problemas. Una de las características principales de este tipo de problemas es que las téc- nicas analíticas estándares de soluciones no son adecuadas para resolverlos. Por esta razón, en este artículo nos centramos en el estudio de los resulta- dos conocidos para los métodos numéricos clásicos y en su adaptación a la resolución de problemas difusos. Resumen.

  6. Pensum No Lineal: Una propuesta innovadora para el diseño de planes de estudio

    Badilla Saxe, Eleonora

    2005-09-01

    Full Text Available El propósito de este artículo, es presentar organizadores conceptuales (como el pensamiento complejo, el aprendizaje significativo y los mapas conceptuales que, con la ayuda de organizadores tecnológicos multimediales (como Internet, la WWW y el CmapTools, permiten el diseño de pensum (programas o planes de estudio no lineales, que evidencien la muti-relacionalidad de sus partes, como una alternativa para la educación en el mundo actual. The purpose of this article is to present conceptual (such as Complex Thinking, Meaningful Learning and Concept Mapping and technological (such as Internet, the WWW and CmapTools organizers that allow a non-linear pensum design that can make visible its multiple interrelations.

  7. Didáctica de la programación lineal con ordenador para economistas.

    Sánchez Álvarez, I.

    1997-01-01

    Full Text Available La generalización de los paquetes informáticos en la enseñanza de la programación lineal ha supuesto transformaciones de gran calado en las técnicas y contenidos docentes. A continuación se recogen aquellos aspectos más relevantes, centrando su análisis en aquellas aplicaciones informáticas de mayor facilidad de uso por considerarlas más adecuadas para la enseñanza en los niveles de licenciatura. De ahí que no se incluyan programas como GAMS que requieren un mayor grado de elaboración por parte del usuario.

  8. Geometría y algebra lineal: talleres resueltos con Matlab

    Franco Arbeláez, Rosa A.

    2007-01-01

    Con el propósito de implementar el uso del derive en los cursos de Algebra lineal surgió la idea de escribir esta guía como una ayuda para los estudiantes en su trabajo con computador. Este folleto contiene guía básica, una serie de ejercicios resueltos con Derive y una colección de prácticas propuestas. En la guía básica presento, además de las principales funciones de Derive en cuanto al manejo de vectores y matrices, los procedimientos usados en los algoritmos más importantes de un curso b...

  9. LA PROGRAMACIÓN LINEAL EN LA ELABORACIÓN DE MEZCLAS DE FERTILIZANTES

    Samuel Rebollar Rebollar; Juvencio Hernández Martínez; Rolando Rojo Rubio; Daniel Cardoso Jiménez; Gabriela Rodríguez-Licea; Eugenio Guzmán-Soria

    2008-01-01

    La Programación Lineal es una importante herramienta matemática que ayuda a resolver problemas de optimización de los recursos escasos. Con el objetivo de generar una recomendación técnico económica que permita maximizar la utilidad proveniente de la fabricación de cuatro mezclas de fertilizantes, sujeta a la disponibilidad y uso de los recursos nitrógeno fósforo y potasio en un periodo de producción (un año), se realizó un trabajo de investigación con información proveniente de un agronegoci...

  10. MÉTODOS ITERATIVOS EFICIENTES PARA RESOLUCIÓN DE SISTEMAS NO LINEALES

    PENKOVA VASSILEVA, MARÍA

    2011-01-01

    El problema de la resolución de ecuaciones y sistemas de ecuaciones no lineales figura entre los más importantes en la teoría y la práctica, no sólo de las matemáticas aplicadas, sino también de muchas ramas de las ciencias, la ingeniería, la física, la informática, la astronomía, las finanzas, . . . El gran número de científicos que han trabajado recientemente en este tema muestran un alto nivel de interés contemporáneo. Aunque el rápido desarrollo de las computadoras digitales llevó a la a...

  11. El método de las ponderaciones en el problema fraccional lineal multiobjetivo

    Hernández Huelin, Mónica; Caballero Fernández, Rafael

    2003-01-01

    Dentro de la programación matemática no lineal, el problema que se ha abordado más en términos teóricos y algorítmicos es el problema convexo. Cuando estamos ante una función fraccional, no tenemos convexidad, pero sí otras buenas propiedades que pueden hacer más o menos fácil la elaboración de algoritmos propios de resolución del problema. En este trabajo nos centramos en adaptar el Método de las Ponderaciones, uno de los métodos clásicos de resolución a priori del problema multiobjetiv...

  12. LINAC quality assurance tool for EPID systems

    Purpose: There are dual purposes for this work: (1) to establish the clinical feasibility of using a commercial LINAC and scanning-liquid ion chamber electronic portal imaging device (SLIC-EPID) for performing quality control checks; and (2) to demonstrate a convenient software tool for performing the tasks. Specifically, our objectives pertain to beam flatness and symmetry, output constancy and enhanced dynamic wedge field verification measurements. Materials and Methods: A Varian C-series accelerator with an SAD of 100 cm was used along with PortalVisionTM Dosimetry Research Mode experimental software. The EPID was calibrated according to the equipment manufacturer's specifications. For output constancy check and flatness and symmetry checks, a portal image was taken at dmax using a 20 x 20 cm2 field for both 6 MV and 18 MV photons. Dose measurements were made at five a priori locations in the image relative to the central axis (one at the central axis, two at either end of the in-plane axis and two at either end of the cross-plane axis). For both output constancy and flatness/symmetry checks, the portal imaging system was operating in normal clinical mode and special dosimetry mode. The central axis value was taken as an average of an array of pixels. The output constancy estimation was established by comparing central axis values over five measurements. Verification of the enhanced dynamic wedge fields occurred with the portal imaging system operating in special dosimetry research mode. Line images were taken at dmax using 15 deg. , 30 deg. , 45 deg. and 60 deg. wedge settings with a field size of 20 x 20 cm2 for both energies. An original delivered wedge profile was established as a reference image and five other images were taken and compared with least-squares analysis to quantify the differences. In order to perform routine LINAC quality checks using a portal imaging system, it must be quick and convenient. However, commercial implementations currently lack

  13. El método de las ponderaciones en el problema fraccional lineal multiobjetivo

    Hernández Huelin, Mónica.

    2003-01-01

    Full Text Available Dentro de la programación matemática no lineal, el problema que se ha abordado más en términos teóricos y algorítmicos es el problema convexo. Cuando estamos ante una función fraccional, no tenemos convexidad, pero sí otras buenas propiedades que pueden hacer más o menos fácil la elaboración de algoritmos propios de resolución del problema. En este trabajo nos centramos en adaptar el Método de las Ponderaciones, uno de los métodos clásicos de resolución a priori del problema multiobjetivo convexo, al caso no convexo de objetivos fraccionales lineales. Dado que no tenemos convexidad ni concavidad de las funciones objetivo, y esta condición es básica para la aplicación de dicho método, estudiaremos este inconveniente con profundidad, estableciendo condiciones bajo las cuales resulta válido este método como generador de los conjuntos eficiente y débilmente eficiente de nuestro problema. Para ello se plantea la necesidad de un estudio detallado de los conceptos de pseudoconvexidad, cuasiconvexidad, invexidad, pseudoinvexidad, etc.. Ofreceremos además un contraejemplo que nos muestra que, si no se dan las condiciones que previamente estableceremos, el Método de las Ponderaciones no es válido para generar todo el conjunto débilmente eficiente de nuestro problema

  14. The Quasi-Linear Solution of Vertical Infiltration; La solucion cuasi-lineal de la infiltracion vertical

    Fuentes, Carlos [Instituto Mexicano de Tecnologia del Agua, Jiutepec, Morelos (Mexico); Parlangue, Jean-Yves [Departamento de Agricultura e Ingenieria Biologica (United States); Haverkamp, Randel; Vauclin, Michael [Laboratorio de Estudio de las Transferencias en Hidrologia y Medio ambiente (France)

    2001-12-01

    The exact solution of the one-dimensional vertical infiltration equation is deducted, when the hydraulic diffusivity is considered constant and the hydraulic conductivity is a combination of both a linear and quadratic functions of the soil water content. This quasi-linear solution includes as particular cases, both the classical solution known as linear soil and the Knight solution. The cumulative infiltrated water as a function of time provided by the quasi-linear solution has been compared with the cumulative infiltrated water obtained from the numerical solution of the Richards equation on three different soils of contrasting hydrodynamic properties. The good agreement between the two solutions has shown that the quasi-linear solution can be used on soils where the accepted hypothesis, on hydraulic diffusivity and hydraulic conductivity, for its deduction is not satisfied. [Spanish] Se deduce la solucion exacta de la ecuacion de la infiltracion unidimensional vertical cuando la difusividad hidraulica es considerada constante y la conductividad hidraulica es una combinacion de una funcion lineal y una cuadratica del contenido volumetrico de agua. Esta solucion cuasi-lineal de la infiltracion contiene, como casos particulares, la solucion clasica conocida como suelo lineal y la solucion de Knight. La lamina infiltrada acumulada en funcion del tiempo proporcionada por la solucion cuasi-lineal se ha comparado con la lamina infiltrada proporcionada por la solucion numerica de la ecuacion de Richards en tres suelos de propiedades hidrodinamicas contrastantes. El buen acuerdo entre las laminas infiltradas ha mostrado que la solucion cuasi-lineal puede utilizarse en suelos donde la difusividad y la conductividad hidraulicas no satisfacen los supuestos de la deduccion.

  15. Development of an Eddy Current Septum for LINAC4

    Barnes, M; Borburgh, J; Fowler, T; Goddard, B; Ueda, A; Weterings, W

    2008-01-01

    A linear accelerator (linac) is the first stage of the CERN accelerator complex. The linac defines the beam quality for subsequent stages of acceleration and the reliability has to be high as a fault of the linac shuts down all other machines. The existing linacs at CERN were designed 30 or more years ago: recent upgrades allowed the linacs to reach LHC requirements but also showed that they are at the limit of their brightness and intensity capabilities. A replacement Superconducting Proton Linac (SPL) has been proposed; the initial part of the SPL is termed LINAC4. The LINAC4 injection bump would be made up of a set of four pulsed dipole magnets; the first of these magnets (BS1) must act as a septum with a thin element dividing the high-field region of the circulating beam from the field-free region through which injected $H^{-}$ beam must pass. The initial specifications for BS1 required; a deflection of 66 mrad at 160 MeV, achieved with a peak field of 628 mT and a length of 250 mm: the field fall time wa...

  16. Transverse quadrupole wake field effects in high intensity linacs

    Transverse quadrupole wake fields exist whenever the beam is not round, and therefore in an alternating-gradient focusing system these fields cannot be eliminated. As a result, these fields represent a potential limitation on high-intensity linac performance. In this note we calculate the magnitude of quadrupole wake field effects for the SLAC linac. (author)

  17. Design of the SLC damping ring to linac transport lines

    The first and second order optics for the damping ring to linac transport line are designed to preserve the damped transverse emittance while simultaneously compressing the bunch length of the beam to that length required for reinjection into the linac. This design, including provisions for future control of beam polarization, is described

  18. MEIC Proton Beam Formation with a Low Energy Linac

    Zhang, Yuhong [Thomas Jefferson National Accelerator Facility, Newport News, VA (United States)

    2015-09-01

    The MEIC proton and ion beams are generated, accumulated, accelerated and cooled in a new green-field ion injector complex designed specifically to support its high luminosity goal. This injector consists of sources, a linac and a small booster ring. In this paper we explore feasibility of a short ion linac that injects low-energy protons and ions into the booster ring.

  19. Induction linac drivers for commercial heavy-ion beam fusion

    This paper discusses induction linac drivers necessary to accelerate heavy ions at inertial fusion targets. Topics discussed are: driver configurations, the current-amplifying induction linac, high current beam behavior and emittance growth, new considerations for driver design, the heavy ion fusion systems study, and future studies. 13 refs., 6 figs., 1 tab

  20. Energy feedback system for the SSRL Injector linac

    The SSRL Injector microwave gun, linac, and booster were commissioned last year. For efficient injection into the booster the linac beam energy must be stable to within about 1%. Unfortunately, fluctuations in the line voltage supplying the unregulated klystron modulators cause fluctuations in the linac beam energy, thus making the operation of the booster potentially very difficult. Without any corrections, the linac energy may drift by as much as one percent per minute or it may jump suddenly by one percent. Fortunately, the linac beam energy can be kept close to the desired value by using feedback on the low level controls of the klystrons feeding two of the linac sections. The energy of the linac is sampled at a beam position monitor (BPM) downstream of the first magnet following the linac. The feedback loop is closed using a low-pass filter that filters out noise from the BPM processing electronics. The feedback is implemented as a computer program (energy feedback) written in C for the SSRL Injector control system, and is robust against various fault conditions, as a result of the many changes and adjustments suggested by the commissioning team who are mentioned in the acknowledgements

  1. Present status of the electron linacs in ISIR, Osaka University

    Nanoscience and Nanotechnology Center, attached to the Institute of Scientific and Industrial Research, Osaka University, was founded in 2002 for developing Bottom-up Nanotechnology, Top-down Nanotechnology, and their Industrial Application. The Radiation Laboratory attached to the center, are conducting management, operation, and maintenance of the 40 MeV L-band electron linac, the 150 MeV S-band electron linac and the 40 MeV laser photo-cathode RF-gun linac. The L-band linac restarted the joint-use from the latter half of 2004 fiscal year after its large-scale upgrade, and 2005 fiscal year became first full-year use after the upgrade. From 2006 fiscal year, in addition to the L-band linac, the S-band linac and the RF-gun linac also began the joint-use in the Osaka University. We report on the present status of three linacs in 2005 fiscal year. (author)

  2. Commissioning of the SPPS Linac Bunch Compressor

    First results and beam measurements are presented for the recently installed linac bunch compressor chicane. The new bunch compressor produces ultra-short electron bunches for the Sub-Picosecond Photon Source (SPPS) and for test beams such as the E164 Plasma Wakefield experiment. This paper will give an overview of the first experiences with tuning and optimizing the compressor together with a description of the beam diagnostics and beam measurements. These measurements form the basis for further detailed study of emittance growth effects such as CSR and wakefields in a previously unmeasured regime of ultra-short bunch lengths

  3. Development of the Medium Energy Linac Systems

    The main purposes of the proton engineering frontier project is developing a proton linac which accelerates 20 mA proton beams up to 100 MeV and supplying 20 MeV and 100 MeV proton beams to the user groups. The project 'Development of the medium energy linac systems' is aiming to design the 100 MeV proton linac, to construct an accelerating cavity, to design a MEBT system, and to develop a energy measurement system. The 100 MeV linac consists of 20 DTL tanks which are operated by five additional klystrons. The focusing lattice is FFDD as the 20 MeV DTL. However the hollow conductors are used for coils of the quadrupole magnets. The shape of the drift tubes in the new tanks is changed to compensate the reduction of the accelerating efficiency in the high energy region. For example, the face angle of drift tubes begins at 40 degrees. The bore radius is selected as 10 mm in order to eliminate beam loss in the beam line. We can obtain the 100 MeV proton beams by using these accelerating structure. We have designed some of the tanks in detail. It covers the modification of the structure by including the stem, post-coupler, and sulg-tuner effects, the error analysis, the thermal and structure analysis, the drift tube design, the magnet design, the various ports design, the support structure design, the end-plate design, etc. Now the first DTL tank is constructed by a local company. An beam extraction system is essential after 20 MeV DTL in order to supply 20 MeV proton beams. Since there are no focusing elements in the structure, the beam should be spread out. The MEBT which consists of two 3-cell DTL tanks is designed to control the beam size in the beam extraction system by magnets in the first tank and to transversely match the beam into the next DTL by magnets in the the second tank. The longitudinal matching is done by the RF in both tanks. We have also developed an energy measurement system using the time of flight method

  4. Beam energy online measurement of BEPCII LINAC

    Wang, Shao-Zhe; Chi, Yun-Long

    2015-01-01

    This paper describes beam energy online measurement of BEPCII linac, presents the calculation formula and some of the results. The method mentioned here measures the beam energy by acquiring beam positions in the horizontal direction with three beam position monitors (BPM) eliminating the effect of orbit fluctuation, which is much better than the one using the single BPM. The error analysis indicates that this online measurement has further potential usage such as a part of beam energy feedback system. The reliability of this method is also discussed and demonstrated in the end of this paper.

  5. A new RFQ linac fabrication technique

    The use of hydrogen furnace brazing has been applied as a joining technology to the fabrication of a Radio-Frequency-Quadrupole (RFQ) linac for the Los Alamos Accelerator Performance Demonstration Facility (APDF). The design concept provides a monolithic cavity with no longitudinal rf, vacuum, or mechanical joints. A 530 MHz, 0.46 meter long engineering model RFQ has been fabricated and tested at the Los Alamos National Laboratory as a technical demonstration of this concept. It is planned that two funneled RFQ's for the APDF (7 MeV, 350 MHz, 100 mAmp CW, each eight meters in length) will be manufactured by this method

  6. Linac based free-electron laser

    A basic treatment of the principle of the linac-driven free-electron laser (FEL) is given. The first part of the paper describes the FEL in low-gain approximation, and in the second part the high-gain FEL theory is given. The majority of the treatment describes FELs in one dimensional approximation, neglecting effects by diffraction of radiation and by electron beam emittance. Only in the final section a few remarks on these issues are given. The ambition of the paper is by no means any progress in FEL theory but a clear presentation of basic FEL theory concepts with explicit derivation of the formulae from first principles. (orig.)

  7. Event Registration System for INR Linac

    The software of the Event registration system for the linear accelerators is described. This system allows receiving of the information on changes of operating modes of the accelerator and supervising of hundreds of key parameters of various systems of the accelerator. The Event registration system consists of the source and listeners of events. The sources of events are subroutines built in existing ACS Linac. The listeners of events are software Supervisor and Client ERS. They are used for warning the operator about change controlled parameter of the accelerator

  8. Design studies of SSC coupled cavity linac

    The SSC coupled cavity linac (CCL) will be a side coupled structure operating at 1284 MHz to accelerate a nominal 25 mA H- beam from 70 MeV to 600 MeV. The authors present results of both cavity design and beam dynamics studies. Each accelerating cavity is optimized by SUPERFISH; coupled cavity characteristics in the region of low-, mid- and high-energies are checked by MAFIA-3D. MAFIA-3D was also used to design the bridge coupler systems. The beam dynamics and error analysis are simulated by CCLDYN and CCLTRACE. Possible future upgrade of the CCL to 1 GeV is also discussed

  9. An induction linac developed for FEL application

    de Mascureau, J.; Anthouard, Ph.; Bardy, J.; Eyharts, Ph.; Eyl, P.; Launspach, J.; Thevenot, M.; Villate, D.

    1992-07-01

    An induction linac is being studied and built at CESTA for FEL application. At first we studied the induction technology and namely the high-voltage (HV) generators and the induction cells. A HV generator designed to feed the cells with calibrated pulses (150 kV, 50 ns, δV/V dispenser cathode. Numerical codes have been developed and simulations have been compared with experimental results for HV generators, induction cells, and the injector. An induction accelerating module has been studied and we plan to have the accelerator working at 3 MeV in 1992.

  10. Fermilab linac upgrade. Module conditioning results

    The 805 MHz side-coupled cavity modules for the Fermilab 400 MeV linac upgrade have been conditioned to accept full power. The sparking rate in the cavities and in the side cells has been reduced to acceptable levels. It required approximately 40 x 106 pulses for each module to achieve an adequately low sparking rate. This contribution outlines the commissioning procedure, presents the sparking rate improvements and the radiation level improvements through the commissioning process and discusses the near-on-line commissioning plans for this accelerator. (Author) ref., 4 figs

  11. Fermilab Linac Upgrade: Module conditioning results

    The 805 MHz Side-coupled cavity modules for the Fermilab 400 MeV linac upgrade have been conditioned to accept full power. The sparking rate in the cavities and in the side-cells has been reduced to acceptable levels. It required approximately 40 x 106 pulses for each module to achieve an adequately low sparking rate. This contribution outlines the commissioning procedure, presents the sparking rate improvements and the radiation level improvements through the commissioning process and disc the near-online commissioning plans for this accelerator

  12. Evaluation of ferromagnetic materials for induction linacs

    For design works of induction linac, it is important to obtain B-H curve of ferromagnetic core materials as a function of magnetization rate. In order to evaluate cost effective induction module, various laminated ferromagnetic materials; silicon steels, amorphous including FINEMET, are magnetized up to 10T/μs. We can conclude that FINEMET is the most excellent materials from the point of core loss, especially at high magnetization rate. From the evaluation of energy loss and heat conduction in the core materials, we conclude that FINEMET cores can operate up to 1 kHz. (author)

  13. Evaluation of ferromagnetic materials for induction linacs

    Hashimoto, Dai; Morimoto, Iwao; Nakajima, Mituo; Horioka, Kazuhiko; Kouno, Toshiyuki [Tokyo Institute of Technology, Department of Energy Science, Meguro, Tokyo (Japan); Zheng, Xiaodong; Maebara, Sunao; Shiho, Makoto [Japan Atomic Energy Research Inst., Tokai, Ibaraki (Japan). Tokai Research Establishment

    2000-03-01

    For design works of induction linac, it is important to obtain B-H curve of ferromagnetic core materials as a function of magnetization rate. In order to evaluate cost effective induction module, various laminated ferromagnetic materials; silicon steels, amorphous including FINEMET, are magnetized up to 10T/{mu}s. We can conclude that FINEMET is the most excellent materials from the point of core loss, especially at high magnetization rate. From the evaluation of energy loss and heat conduction in the core materials, we conclude that FINEMET cores can operate up to 1 kHz. (author)

  14. Short wavelength FELs using the SLAC linac

    We have studied the use of the SLAC linac to drive FELs at wavelengths down to a few Angstroms. Lasing would be achieved in a single pass of a low emittance, high peak current, high energy electron beam through a long undulator by Self-Amplified-Spontaneous-Emission (SASE). About 1013 photons per pulse can be produced in 100 fs pulses at a 120 Hz rate, corresponding to brightness levels of about 1022 average and 1032 peak. Peak power level are tens of GW. Electron energies of 10-20 GeV are required. Significant improvement of FEL performance seems possible using harmonic generation techniques according to results from numerical simulations

  15. Upgrade of kek linac control network system

    KEK Linac has been supplying a stable beam to the ring four different. In order to provide a highly available beam over a long period of time, a stable network communication between the server computer and the local control device is essential. By the Great East Japan Earthquake of 2011, part of the network system were damaged. Further, because it promotes the advancement of injector toward SuperKEKB, was performed updates to the network system with high reliability and high performance. In this paper, I will report more information about network monitoring system and update of network system. (author)

  16. Linac design for the LCLS project at SLAC

    The Linac Coherent Light Source (LCLS) at SLAC is being designed to produce intense, coherent 0.15-nm x-rays. These x-rays will be produced by a single pass of a 15 GeV bunched electron beam through a long undulator. Nominally, the bunches have a charge of 1 nC, normalized transverse emittances of less than 1.5π mm-mr and an rms bunch length of 20 μm. The electron beam will be produced using the last third of the SLAC 3-km linac in a manner compatible with simultaneous operation of the remainder of the linac for PEP-II. The linac design necessary to produce an electron beam with the required brightness for LCLS is discussed, and the specific linac modifications are described

  17. Photon and photoneutron spectra produced in radiotherapy 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 Bremsstrahlung spectra show the same features regardless of the linac voltage. The amount of photons and neutrons produced by the 15 MV linac is smaller than that found for the 18 MV linac. As expected, Bremsstrahlung spectra ends according to the voltage used to accelerate the electrons. (Author)

  18. Photon and photoneutron spectra produced in radiotherapy Linacs

    Vega C, H. R. [Universidad Autonoma de Zacatecas, Unidad Academica de Estudios Nucleares, Calle Cipres No. 10, Fracc. La Penuela, 98068 Zacatecas (Mexico); Martinez O, S. A. [Universidad Pedagogica y Tecnologica de Colombia, Grupo de Fisica Nuclear Aplicada y Simulacion, Av. Central del Norte Km. 1, Via Paipa Tunja, Boyaca (Colombia); Benites R, J. L. [Universidad Autonoma de Nayarit, Postgrado CBAP, Carretera Tepic Compostela Km. 9, Xalisco, Nayarit (Mexico); Lallena, A. M., E-mail: fermineutron@yahoo.com [Universida de Granada, Departamento de Fisica Atomica, Molecular y Nuclear, E-18071 Granada (Spain)

    2011-10-15

    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{sup -6} and 1 MeV. Neutron and Bremsstrahlung spectra show the same features regardless of the linac voltage. The amount of photons and neutrons produced by the 15 MV linac is smaller than that found for the 18 MV linac. As expected, Bremsstrahlung spectra ends according to the voltage used to accelerate the electrons. (Author)

  19. A compact high-power proton linac for radioisotope production

    Conventional designs for proton linacs use a radiofrequency quadrupole (RFQ), followed by a drift-tube linac (DTL). For higher final beam energies, a coupled cavity linac (CCL) follows the DTL. A new structure, the coupled-cavity drift-tube linac (CCDTL) combines features of an Alvarez DTL and the CCL. Operating in a π/2 structure mode, the CCDTL replaces the DTL and part of the CCL for particle velocities in the range 0.1 < β < 0.5. The authors present a design concept for a compact linac using only an RFQ and a CCDTL. This machine delivers a few mA of average beam current at a nominal energy of 70 MeV and is well suited for radioisotope production

  20. Present status of KEK electron/positron Linac

    The Electron/Positron Linac injects electron and positron beams into four different rings; KEKB High Energy Ring(electron 8GeV), KBKB Low Energy Ring(positron 3.45 GeV), PF(electron 2.5 GeV), PF-AR(electron 2.5 GeV). During the summer shutdown of 1999, many improvements such as upgrade of an SHB1 power supply, installation of a new SHB2 cavity with an improved cooling channel, introduction of a new workstation for feedback systems etc.. Stability of the linac has been improved and beam switching among these rings is performed in a short time. Operation time of the linac during FY 1999 was 7,296 hours. Statistics of linac operation and activities for obtaining high reliability of the linac are presented. (author)

  1. 10MeV 25KW industrial electron LINAC

    Kamino, Y.

    1998-06-01

    A 10MeV 25KW plus class electron LINAC was developed for sterilisation of medical devices. The LINAC composed of a standing wave type single cavity prebuncher and a 2m electro-plated travelling wave guide uses a 5MW 2856MHz pulse klystron as an RF source and provides 25KW beam power at the Ti alloy beam window stably after the energy analysing magnet with 10MeV plus-minus 1 MeV energy slit. The practical maximum beam power reached 29 KW and this demonstrated the LINAC as one of the most powerful S-band electron LINACs in the world. The control of the LINAC is fully automated and the "One-Button Operation" is realised, which is valuable for easy operation as a plant system. 2 systems have been delivered and are being operated stably.

  2. Aplicación de perturbaciones cúbicas a sistemas lineales controlados por realimentación de estados = Application of cubic disturbances to linear systems controlled by state feedback

    Piarpuzán Estupiñán, Diego Fernando

    2011-01-01

    En este trabajo se presenta la aplicación de perturbaciones cúbicas sobre sistemas dinámicos lineales SISO y MIMO, lineales, continuos e invariantes en el tiempo, controlados por realimentación de estados; diseñando finalmente una ley de control no lineal uNL(t). El diseño de la ley de control no lineal uNL(t) se aplica inicialmente sobre un sistema lineal SISO, estableciendo algunas condiciones básicas sobre los parámetros de la ley de control, con el objetivo de disminuir el esfuerzo de con...

  3. RIA Superconducting Drift Tube Linac R & D

    J. Popielarski; J. Bierwagen; S. Bricker; C. Compton; J. DeLauter; P. Glennon; T. Grimm; W. Hartung; D. Harvell; M. Hodek; M. Johnson; F. Marti; P. Miller; A. Moblo; D. Norton; L. Popielarski; J. Wlodarczak; R. C. York; A. Zeller

    2009-05-22

    Cavity and cryomodule development work for a superconducting ion linac has been underway for several years at the National Superconducting Cyclotron Laboratory. The original application of the work was the proposed Rare Isotope Accelerator. At present, the work is being continued for use with the Facility for Rare Isotope Beams (FRIB). The baseline linac for FRIB requires 4 types of superconducting cavities to cover the velocity range needed to accelerate an ion beam to 200 MeV/u: 2 types of quarter-wave resonator (QWR) and 2 types of half-wave resonator (HWR). Superconducting solenoids are used for focussing. Active and passive shielding is required to ensure that the solenoids’ field does not degrade the cavity performance. First prototypes of both QWR types and one HWR type have been fabricated and tested. A prototype solenoid has been procured and tested. A test cryomodule has been fabricated and tested. The test cryomodule contains one QWR, one HWR, one solenoid, and one super-ferric quadrupole. This report covers the design, fabrication, and testing of this cryomodule

  4. SNS Linac Modulator Operational History And Perfomance

    Fourteen High Voltage Converter Modulators (HVCM) were initially installed at the Spallation Neutron Source Linear Accelerator (SNS Linac) at the Oak Ridge National Laboratory in 2005. A fifteenth HVCM was added in 2009. Each modulator provides a pulse of up to 140 kV at a maximum width of 1.35 msec. Peak power level is 11 MW with an 8% duty factor. The HVCM system must be available for neutron production (NP) 24/7 with the exception being two, 6-week maintenance periods per year. HVCM reliability is one of the most important factors to maximize Linac availability and achieve SNS performance goals. During the last few years several modifications have been implemented to improve the overall system reliability. This paper presents operational history of the HVCM systems and examines failure mode statistical data since the modulators began operating at 60 Hz. System enhancements and upgrades aimed at providing long term reliable operation with minimal down time are also discussed in the paper.

  5. Linac-driven spallation-neutron source

    Strong interest has arisen in accelerator-driven spallation-neutron sources that surpass existing facilities (such as ISIS at Rutherford or LANSCE at Los Alamos) by more than an order of magnitude in beam power delivered to the spallation target. The approach chosen by Los Alamos (as well as the European Spallation Source) provides the full beam energy by acceleration in a linac as opposed to primary acceleration in a synchrotron or other circular device. Two modes of neutron production are visualized for the source. A short-pulse mode produces 1 MW of beam power (at 60 pps) in pulses, of length less than 1 ms, by compression of the linac macropulse through multi-turn injection in an accumulator ring. A long-pulse mode produces a similar beam power with 1-ms-long pulses directly applied to a target. This latter mode rivals the performance of existing reactor facilities to very low neutron energies. Combination with the short-pulse mode addresses virtually all applications

  6. Computation of Normal Conducting and Superconducting Linear Accelerator (LINAC) Availabilities

    A brief study was conducted to roughly estimate the availability of a superconducting (SC) linear accelerator (LINAC) as compared to a normal conducting (NC) one. Potentially, SC radio frequency cavities have substantial reserve capability, which allows them to compensate for failed cavities, thus increasing the availability of the overall LINAC. In the initial SC design, there is a klystron and associated equipment (e.g., power supply) for every cavity of an SC LINAC. On the other hand, a single klystron may service eight cavities in the NC LINAC. This study modeled that portion of the Spallation Neutron Source LINAC (between 200 and 1,000 MeV) that is initially proposed for conversion from NC to SC technology. Equipment common to both designs was not evaluated. Tabular fault-tree calculations and computer-event-driven simulation (EDS) computer computations were performed. The estimated gain in availability when using the SC option ranges from 3 to 13% under certain equipment and conditions and spatial separation requirements. The availability of an NC LINAC is estimated to be 83%. Tabular fault-tree calculations and computer EDS modeling gave the same 83% answer to within one-tenth of a percent for the NC case. Tabular fault-tree calculations of the availability of the SC LINAC (where a klystron and associated equipment drive a single cavity) give 97%, whereas EDS computer calculations give 96%, a disagreement of only 1%. This result may be somewhat fortuitous because of limitations of tabular fault-tree calculations. For example, tabular fault-tree calculations can not handle spatial effects (separation distance between failures), equipment network configurations, and some failure combinations. EDS computer modeling of various equipment configurations were examined. When there is a klystron and associated equipment for every cavity and adjacent cavity, failure can be tolerated and the SC availability was estimated to be 96%. SC availability decreased as

  7. Linac4 crosses the 100 MeV threshold

    Corinne Pralavorio

    2016-01-01

    The new linear accelerator, which from 2020 will be the first link in the accelerator chain, has entered a new stage of its commissioning.   Members of the team in charge of the commissioning of Linac4 in the accelerator’s control room. A few hours earlier, Linac4 accelerated a beam to 107 MeV for the first time. We couldn’t have imagined a more appropriate date: on 1 July (1.07), Linac4 reached an energy of 107 MeV. Having crossed the 100 MeV barrier, the linear accelerator is now on the home straight of its commissioning. “This stage was very quick – it took less than two weeks,” says Alessandra Lombardi, deputy project leader of Linac4, in charge of the commissioning. In 2020, Linac4 will replace the existing Linac2 as the first link in the accelerator chain. It will accelerate beams of H- ions (protons surrounded by two electrons) to 160 MeV, compared to 50 MeV with Linac2. The new machine is particularly sophisticated as it comprises...

  8. First Linac4 DTL & CCDTL cavities installed in tunnel

    Katarina Anthony

    2014-01-01

    On 5 June, the first Drift Tube Linac (DTL) was successfully transported to its forever home in the Linac4 tunnel. Similarly, the first Cell-Coupled Drift Tube Linac (CCDTL) was installed on 6 June. These moves marked the end of years of design and manufacturing by Linac4 teams.   Although it may seem like a relatively routine transport operation, the DTL's move was a landmark event for the entire Linac4 collaboration. "Along with the first four Cell-Coupled DTL modules, which were installed on the following two working days, these are the first accelerating structures after front-end commissioning to be installed in the tunnel," says Frank Gerigk, who is responsible for all Linac4 accelerating structures. "It is a major milestone, because work on all these structures started well over a decade ago." The transport operation was also quite a victory for the Linac4 DTL team, whose journey to a complete DTL structure has been a bit of a wild ride. &qu...

  9. Alignment and Field Error Tolerance in Linac4

    Bellodi, G; Garcia Tudela, M; Hein, L; Lallement, J B; Lanzone, S; Lombardi, A M; Posocco, P; Sargsyan, E

    2011-01-01

    LINAC4 [1] is a linear accelerator for negative Hydrogen ions (H−), which will replace the 50 MeV proton LINAC (LINAC2) as linear injector for the CERN accelerators. The higher output energy (160 MeV) together with charge-exchange injection will allow increasing beam intensity in the following machines. LINAC4 is about 80 m long, normal-conducting, and will be housed in a tunnel 12 m below ground on the CERN Meyrin site. The location has been chosen to allow using LINAC4 as the first stage of acceleration for a Multi-MegaWatt superconducting LINAC (SPL [2]). A 60 m long transfer line brings the beam towards the present LINAC2-to-PS Booster transfer line, which is joined at the position of BHZ20. The new transfer line consists of 17 new quadrupoles, an RF cavity and 4 bending magnets to adjust both the direction and the level for injection into the PS Booster. End-to-end beam dynamics simulations have been carried out in parallel with the codes PATH [3] and TRACEWIN[4]. Following the definition of the layout...

  10. The Superconducting Proton Linac plasma generator and Linac4 H-Ion source

    Full text: In the course of the sLHC project, CERN is studying a new plasma generator for the Superconducting Proton Linac (SPL) similar to the RF driven volume H- source of Linac4. The new plasma generator has been designed for a higher duty factor of up to 6% and has therefore been equipped with several cooling systems for the ceramic plasma chamber, ignition element, extraction area, RF antenna and matching network. This resulted in a redesign of the magnetic cusp configuration which had to be displaced and reinforced by the use of Halbach magnets which are now protected against heating due to RF induced eddy currents by an effective copper shielding. The Teststand of the plasma generator and its RF generator have been commissioned and thorough measurements are performed, including the plasma's light spectrum, thermal imaging of the source, RF-plasma coupling characterisation and Langmuir probe measurements of the plasma. (author)

  11. Injection schemes for the TOP Linac; Schemi di iniezione per il TOP Linac

    Picardi, L.; Ronsivalle, C. [ENEA, Centro Ricerche Frascati, Frascati, RM (Italy). Dipt. Innovazione; Bartolini, R. [Istituto Superiore di Sanita' , Rome (Italy)

    1999-07-01

    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. [Italian] In questo rapporto sono studiati due schemi di iniezione nella sezione accelerante SCDTL a 3 GHz del TOP (terapia oncologica con protoni) linac del fascio di protoni generato da un acceleratore lineare di 7 MeV. L'acceleratore e' frutto di una convenzione tra L'ENEA e l'Istituto Superiore di Sanita'. Rispetto a versioni precedenti del progetto, viene eliminato il vincolo della sincronizzazione delle radiofrequenze dei due acceleratori.

  12. Development of the low energy linac systems

    The project 'Development of the Low Energy Linac System' is aiming to develop the 20 MeV proton linac system. This consists of a 50 keV proton injector, a 3 MeV RFQ, and a 20 MeV DTL. We obtained the first beam signal after the 20 MeV linac. The high power switch installed in the ion source supplies the pulsed beam into the following LEBT. The pulse operation was successfully tested. The main role of the LEBT is to match the beam into the 3 MeV RFQ. The total length of the four-vane type RFQ is about 3.26m. For the field stabilization, we used the resonant coupling scheme and dipole stabilizer rods. An 1 MW klystron supplies the RF power into the RFQ. After tuning, the field deviation of the quadrupole mode is less than 2% of the design value and the dipole fraction is less than 5% of the operating mode. The following accelerating structure is DTL which accelerate 20 mA proton beams up to 20 MeV. It consists of 4 tanks and the length of each tank is less than 5 m. The lattice is FFDD type and the integrated fields of the quadrupole magnets are 1.75 T. The inner walls of the tanks are copper-plated by PR plating method. The thickness is 100m with the roughness of 0.3m. Each drift tube consists of 6 parts and assembled by e-beam welding. The tanks and drift tubes are aligned under the installation limit of 50m by using the laser-tracker. The tuning by the slug tuners and post couplers results in the field uniformity of 2% and field sensitivity of 100%/MHz. In order to detect the beam signal, we installed the Faraday cup after the RFQ or the DTL. For the RFQ, we observed the beam of 12 A under the forward RF power of 450 kW. The beam current after DTL is about 0.5 A when RF power of 150 kW was fed into each tank

  13. Análisis no lineal de mallas espaciales de doble capa

    Estévez Cimadevila, Francisco Javier

    1991-04-01

    Full Text Available This paper is related to the topic developed in my RH.D. thesis. A new model is proposed to describe the non-linear behaviour of straight pin-jointed compression members. Sucti a method Is based upon obtaining the complete constitutive equations in the case of circular hollow sections. The stability functions of imperfect bars and the analytical formulation of the post-buckiing behaviour are obtained by taking the exact expression of the curvature in the integratlon of the differential equation of the elastic. The linearization of the constitutive relationships and the application of an incremental iterative model based upon the modification of the elasticity of the bars at critical point allows us to consider the non-linear analysis of the double layer space grids. The models of analysis proposed here have been applied to a wide variety of trusses with different characteristics and typologies, some examples of which accompany this paper.

    Este artículo corresponde al tema de investigación desarrollado en mi tesis doctoral. Se plantea un nuevo modelo para describir el comportamiento no lineal de piezas rectas biarticuladas sometidas a compresión, basado en la obtención de las ecuaciones constitutivas en el caso de los perfiles tubulares huecos de sección circular. Se obtienen las funciones de estabilidad de barras imperfectas y la formulación analítica del comportamiento postpandeo tomando la expresión exacta de la curvatura en la integración de la ecuación diferencial de la elástica. La linearización de las leyes constitutivas y la aplicación de un modelo incremental Iterativo basado en la modificación del módulo de elasticidad de las barras en estado crítico permite abordar el análisis no lineal de las mallas espaciales de doble capa. Los modelos de análisis propuestos se aplicaron a una amplia variedad de mallas de diversas tipologías y características de las que se acompañan algunos ejemplos en el artículo.

  14. High-power linac for the spallation neutron source

    Rej, D. J. (Donald J.)

    2004-01-01

    The Spallation Neutron Source (SNS) will be the world's most intense source of neutrons for fundamental science and industrial applications. In this paper, we review the physics requirements, design, construction, installation, and first commissioning results of the 1-GeV, 1.4-MW average power RF linac for SNS. The overall project is 82% complete, with most of the linac hardware manufactured and delivered to the SNS site. Commissioning of the first drift tube linac tanks was a success. Approximately 100% of the beam was transmitted at full average current while achieving the emittance goal of less than 0.3 {pi} mm-mrad.

  15. Status of Superconducting RF Linac Development for APT

    Chan, K. C. D.; Campbell, B. M.; Gautier, D. C.; Gentzlinger, R. C.; Gioia, J. G.; Haynes, W. B.; Katonak, D. J.; Kelley, J. P.; Krawczyk, F. L.; Madrid, M. A.; Mitchell, R. R.; Montoya, D. I.; Schmierer, E. N.; Schrage, D. L.; Shapiro, A. H.

    2000-01-01

    This paper describes the development progress of high current superconducting RF linacs in Los Alamos, performed to support a design of the linac for the APT (Accelerator Production of Tritium) Project. The APT linac design includes a CW superconducting RF high energy section, spanning an energy range of 211 to 1030 MeV, and operating at a frequency of 700 MHz with two constant beta sections (beta of 0.64 and 0.82). In the last two years, we have progressed towards build a cryomodule with bet...

  16. History of the JAERI linac facility for 33 years

    The JAERI electron linear accelerator will be shutdown and disassembled at the end of 1993. At the JAERI, a prototype 20 MeV linac was constructed at 1960, and was used for the neutron time-of-flight experiments and for the isotope productions. An upgraded 120 MeV linac was constructed at 1972, and was used for many fields of research works until 1993. History of the JAERI Linac and the results of the works made using these facilities are reviewed, and also R/D on the accelerator engineering are described briefly. (author)

  17. R&D Energy Recovery Linac at Brookhaven National Laboratory

    Litvinenko, Vladimir; Beavis, D.; Ben-Zvi, Ilan; Blaskiewicz, Michael; Burrill, Andrew; Calaga, Rama; Cameron, Peter; Chang, Xiangyun; Drees, K.A.; Ganetis, G.; Gamble, Michael; Hahn, H.; Hammons, L.R.; Hershcovitch, A.; Hseuh, H.C.; Jain, A.K.; Kayran, A.; Kewisch, Jorg; Lambiase, R.F.; Lederle, D.L.; Mahler, G.J.; McIntyre, G.; Meng, W.; Nehring, T.C.; Oerter, B.; Pai, C.; Pate, D.; Phillips, Daniel; Pozdeyev, Eduard; Rao, Triveni; Reich, J.; Roser, Thomas; Russo, T.; Smith, K.; Tuozzolo, Joseph; Weiss, D.; Williams, N.W.W.; Yip, Kin; Zaltsman, A.; Bluem, Hans; Cole, Michael; Favale, Anthony; Holmes, D.; Rathke, John; Schultheiss, Tom; Delayen, Jean; Funk, L.; Phillips, H.; Preble, Joseph

    2008-07-01

    Collider Accelerator Department at BNL is in the final stages of developing the 20-MeV R&D energy recovery linac with super-conducting 2.5 MeV RF gun and single-mode super-conducting 5-cell RF linac. This unique facility aims to address many outstanding questions relevant for high current (up to 0.5 A of average current), high brightness energy-recovery linacs with novel Zigzag-type merger. We present the performance of the R&D ERL elements and detailed commissioning plan.

  18. A new method for improving beam quality of LINAC

    The principle of the self-adaptive feed-forward (SAFF) control to improve the beam quality of linac is introduced. the analytical procedure for calculating the control signals, the structure of a practical control system, and applications of SAFF in klystron, RF gun, and linac are presented, especially the application in the thermionic gun whose response is non-linear, time-variant and of large time-delay. The described control system is operational and some primary experimental results have been obtained, including the control of amplitude and phase fluctuations of the klystron output, the microwave field in the gun cavity and linac

  19. Initial operation of the Argonne superconducting heavy-ion linac

    Initial operation and recent development of the Argonne superconducting heavy-ion linac are discussed. The linac has been developed in order to demonstrate a cost-effective means of extending the performance of electrostatic tandem accelerators. The results of beam acceleration tests which began in June 1978 are described. At present 7 of a planned array of 22 resonators are operating on-line, and the linac system provides an effective accelerating potential of 7.5 MV. Although some technical problems remain, the level of performance and reliability is sufficient that appreciable beam time is becoming available to users

  20. Development of RF linac for high-current applications

    Chan, K.C.D.; Lawrence, G.P.; Schneider, J.D.

    1997-12-31

    High-current proton linacs are promising sources of neutrons for material processing and research applications. Recently, a linac design that makes use of a combination of normal-conducting (NC) and superconducting (SC) linac technologies has been proposed for the US Accelerator Production of Tritium Project. As a result, a multi-year engineering development and demonstration (ED and D) program is underway. In this paper, the authors will describe the design and merits of the NC/SC hybrid approach. The scope, technology issues, and present status of the ED and D Program, and the participation of industry will also be described.

  1. Using basic electromagnetism to introduce LINAC4 (CERN)

    Cid-Vidal, Xabier; Cid, Ramon; Vretenar, Maurizio

    2016-07-01

    The LHC is the last element of CERN’s accelerator complex, which is a succession of machines with increasingly higher energies. Everything starts in the 50 MeV linear accelerator (LINAC2), but a new linear accelerator, the 160 MeV LINAC4, will replace LINAC2 in 2018, upgrading LHC injectors to higher intensity and eventually increasing the luminosity of LHC. The aim of this article is briefly introducing this new accelerator, and presenting a simple application of some fundamental laws of magnetism to be taken to the secondary school classrooms.

  2. Los modos de pensar el álgebra lineal y ejemplos AD HOC en problemas específicos de su enseñanza y aprendizaje

    González, Marcela

    2013-01-01

    Se presenta un análisis de distintos hechos didácticos específicos en el álgebra lineal, a través de dos ejemplos. El primero se aborda, bajo el enfoque de la teoría de los modos de pensar el álgebra lineal de Anna Sierpinska (sintético-geométrico, analítico-aritmético y analítico-estructural) para indagar cómo estudiantes universitarios se enfrentan a los conceptos dependencia e independencia lineal de vectores y de solución de un sistema de ecuaciones lineales en R2 y R3. El segundo ejemplo...

  3. Extracción crosslingüe de documentos usando mapas semánticos no-lineales

    Banchs Martínez, Rafael Enrique; Ruiz Costa-Jussà, Marta

    2009-01-01

    Se propone un procedimiento no-lineal de mapeado semántico para extraer información multilingüe. El método consiste en utilizar una técnica de reducción de espacio no-lineal para agrupar colecciones de documentos multilingües. En el método propuesto, se construyen para cada lengua agrupaciones independientes de la colección multilingüe y se usan las similitudes de las expresiones semánticas para extraer documentos multilingües. Se implementan dos variantes del método y se comparan con técnica...

  4. Wall current monitor for SPring-8 linac

    A fast rise time, broad band width and wide dynamic range wall current monitor was developed for SPring-8 linac. The performances are a rise time of ∼250ps, an effective impedance of 1.4Ω (output of ∼1.4V/A) and a bandwidth of 18kHz-2GHz. From a result of examination using 40ns electron beam, a significant change of effective impedance was not observed when a peak current was changed up to 12A or when a beam was moved by 8mm in a vacuum pipe. A circuit model that includes a core inductor loop was constructed. Using this model effective impedance and band width were calculated and compared to measured ones. They agreed very well except one part. In consequence the mechanism of wall current monitor can be explained by means of this model. (author)

  5. The injector linac for the Mainz microtron

    The design and setup of a 3.5 MeV, 100μA injector for a cascade of race track microtrons is presented. It replaces a 2.1 MeV Van De Graaff for getting higher reliability, improved beam dynamics in the first RTM by increased and more stable input energy, as well as an easier access and a better vacuum to launch a beam of polarized electrons. In this paper, the considerations which led under given boundary conditions to the final design concept are discussed and its realization with PARMELA is described. Details of the linac setup are given. First operation showed a good longitudinal performance (energy stability ≤ ±2 star 10-4, spectrum ≤ 1 star 10-3 FWHM, bunch length ≤ ± 1.5 degrees) and an excellent reproducibility of machine operation

  6. High power switches for ion induction linacs

    The success of linear induction ion accelerators for accelerator inertial fusion (AIF) applications depends largely on innovations in pulsed power technology. There are tight constraints on the accuracy of accelerating voltage waveforms to maintain a low momentum spread. Furthermore, the non-relativistic ion beams may be subject to a klystron-like interaction with the accelerating cavities leading to enhanced momentum spread. In this paper, the author describe a novel high power switch with a demonstrated ability to interrupt 300 A at 20 kV in less than 60 ns. The switch may allow the replacement of pulse modulators in linear induction accelerators with hard tube pulsers. A power system based on a hard tube pulser could solve the longitudinal instability problem while maintaining high energy transfer efficiency. The problem of longitudinal beam control in ion induction linacs is reviewed in Section 2. Section 3 describes the principles of the plasma flow switch. Experimental results are summarized in Section 4

  7. High power pulse modulator for PLS LINAC

    Complete design, assembly, and testing of 200 MW modulators are in progress at Pohang Accelerator Laboratory (PAL) for the full energy injection linac system of the Pohang Light Source (PLS). A 150-MW pre-prototype modulator (350 kV, 3.5 μs flat-top width, and 840 Ω load) has been assembled and tested up to 175 MW. Design, construction, and test of a 200-MW prototype modulator (400 kV, 4.4 μs flat-top width, 800 Ω load) has also been completed. Eleven units of main 200-MW modulators are under construction, and their assembly is expected to be completed in 1993. This paper presents the design and the current status of performance results of 150-MW and 200-MW modulators

  8. Design considerations on a proton superconducting linac

    The authors analyze the longitudinal motion of a single proton in a superconducting linear accelerator. They derive the linearized equations of motion, and develop a matrix formalism to represent the progress of motion. The goal is to provide a tool which can be easily included in a computer code for the design of superconducting proton linacs. In particular they determine the stability conditions, and the amount of motion mismatch resulting from the presence of drift insertions, and from the rate of acceleration. Space-charge effects have not been included in the analysis. They complement the analysis with considerations of the rf and cryogenic power requirements, of the pulsed mode of operation, and of the beam transverse confinement. They conclude with an example of a Spallation Neutron Source

  9. Energy Recovery Linacs for Light Source Applications

    George Neil

    2011-04-01

    Energy Recovery Linacs are being considered for applications in present and future light sources. ERLs take advantage of the continuous operation of superconducting rf cavities to accelerate high average current beams with low losses. The electrons can be directed through bends, undulators, and wigglers for high brightness x ray production. They are then decelerated to low energy, recovering power so as to minimize the required rf drive and electrical draw. When this approach is coupled with advanced continuous wave injectors, very high power, ultra-short electron pulse trains of very high brightness can be achieved. This paper will review the status of worldwide programs and discuss the technology challenges to provide such beams for photon production.

  10. Radiation processing with the Messina electron linac

    Auditore, L.; Barnà, R. C.; De Pasquale, D.; Emanuele, U.; Loria, D.; Morgana, E.; Trifirò, A.; Trimarchi, M.

    2008-05-01

    In the last decades radiation processing has been more and more applied in several fields of industrial treatments and scientific research as a safe, reliable and economic technique. In order to improve existing industrial techniques and to develop new applications of this technology, at the Physics Department of Messina University a high power 5 MeV electron linac has been studied and set-up. The main features of the accelerating structure will be described together with the distinctive features of the delivered beam and several results obtained by electron beam irradiations, such as improvement of the characteristics of polymers and polymer composite materials, synthesis of new hydrogels for pharmaceutical and biomedical applications, reclaim of culture ground, sterilization of medical devices, development of new dosimeters for very high doses and dose rates required for monitoring of industrial irradiations.

  11. RF control of ICR proton linac

    At the ICR Kyoto University, the proton linac has been developed. The RF high power is fed into the cavity from the klystron and the RF pulse width is 65 μsec. The RF amplitude and the phase in the cavity are affected by the beam loading and the pulse shape of the klystron cathode voltage. The fast RF stabilization system are required to accelerate the high beam stably. The stabilization system consists of the auto level control (ALC) and the phase locked loop (PLL). The designed band width is more than 1 MHz. The main modules of the circuit are the PIN diode attenuator, the fast phase detector, the phase shifter and the wideband feedback amplifier. The variation of the RF amplitude and the RF phase are 0.5 % with ALC and 5deg with PLL, respectively. (author)

  12. FRIB driver linac vacuum model and benchmarks

    Durickovic, Bojan; Kersevan, Roberto; Machicoane, Guillaume

    2014-01-01

    The Facility for Rare Isotope Beams (FRIB) is a superconducting heavy-ion linear accelerator that is to produce rare isotopes far from stability for low energy nuclear science. In order to achieve this, its driver linac needs to achieve a very high beam current (up to 400 kW beam power), and this requirement makes vacuum levels of critical importance. Vacuum calculations have been carried out to verify that the vacuum system design meets the requirements. The modeling procedure was benchmarked by comparing models of an existing facility against measurements. In this paper, we present an overview of the methods used for FRIB vacuum calculations and simulation results for some interesting sections of the accelerator. (C) 2013 Elsevier Ltd. All rights reserved.

  13. Error sensitivity analysis of drift tube linac

    The Drift Tube Linac (DTL) is used for acceleration of protons and ions in beta range of 0.04 to 0.4. It is a RF resonating cavity excited in TM0.10 mode wherein E-field is along the axis and H-field is along azimuth. The DTL consists of array of Drift tubes which performs dual function of shielding the accelerating beam from negative RF phase and for housing the magnetic lenses for transverse focusing of the beam. The axial gaps between DTs are called acceleration gaps as particle sees E-field in this gap. The accelerating beam profile is dependent on high frequency E-field and H-field spatial distribution and static magnetic field generated by the PMQs. However the Electromagnetic fields (both static and dynamic) are expected to deviate from ideal due to fabrication tolerances and will vary during operations due to temperature fluctuations which results in mechanical deformation in the RF structures, The static magnetic field generated by PMQs will vary from PMQ to PMQ due to variation in properties of permanent magnets. This paper describes the results of sensitivity analysis on accelerating charged particle beam in Drift Tube linac due to mechanical deformations in the RF structures, variations of amplitude and phase of RF power, variation of ∫G.dl and uniformity of ∫G.dl, roll angle of PMQs and misalignment of magnetic lenses. Results obtained from simulations carried out using COMSOL, CST, Super fish and Tracewin are used to conclude effective deviations in the beam phase space and energy gain due to above mentioned factors. This analysis is carried out on 10 MeV to 20 MeV section of DTL for LEHIPA. (author)

  14. A Program for Optimizing SRF Linac Costs

    Powers, Thomas J. [JLAB

    2013-04-01

    Every well-designed machine goes through the process of cost optimization several times during its design, production and operation. The initial optimizations are done during the early proposal stage of the project when none of the systems have been engineered. When a superconducting radio frequency (SRF) linac is implemented as part of the design, it is often a difficult decision as to the frequency and gradient that will be used. Frequently, such choices are made based on existing designs, which invariably necessitate moderate to substantial modifications so that they can be used in the new accelerator. Thus the fallacy of using existing designs is that they will frequently provide a higher cost machine or a machine with sub-optimal beam physics parameters. This paper 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 [1] several years ago while they were in the process of developing a conceptual design for the New Light Source project. 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.

  15. Algoritmo urza para el análisis de sensibilidad en problemas de programación lineal

    Zamanillo Elguezabal, Ibon; Uría Aróstegui, Victor; Larrañaga Lesaca, Jesús M.

    2004-01-01

    Este artículo menciona que el algoritmo pretende llenar un hueco existente en los análisis de sensibilidad de la Programación Lineal. Estos análisis abarcan tradicionalmente a todos los coeficientes del sistema excepto a los coeficientes técnicos de las variables de la BASE, debido a la dificultad de calcular la inversa de ésta cuando se ha introducido un parámetro en uno de sus elementos.

  16. Modelo lineal generalizado y cálculo de la provisión técnica

    Boj del Val, Eva; Costa Cor, Teresa

    2014-01-01

    En este material se recogen características básicas del modelo lineal generalizado y su aplicación al cálculo de provisiones técnicas. Se explica cómo el modelo clásico Chain-Ladder se obtiene como caso particular y se detalla el cálculo del error de predicción y de la distribución predictivas de las reservas mediante bootstrap.

  17. Paquete VilGebra: recurso didáctico a través del uso del software Mathematica en el campo del álgebra lineal

    Vílchez, Enrique

    2015-01-01

    VilGebra es un paquete elaborado por el autor de esta propuesta, que añade al software comercial Mathematica 9, ochenta y seis comandos para desarrollar distintos procedimientos vinculados con un curso introductorio de álgebra lineal para ingeniería. En general, las instrucciones integradas en VilGebra recorren ejes temáticos relacionados con: matrices y determinantes, vectores en R, rectas y planos, espacios vectoriales reales, proyecciones ortogonales, transformaciones lineales, valores y v...

  18. Avaliação do bis(4-metilfenilditiocarbimatozincato(II de tetrabutilamônio como acelerador no processo de vulcanização do elastômero polibutadieno Evaluation of [tetrabutyl ammonium bis(4-methylphenyldithiocarbimatezincate-2] as accelerator in vulcanization process of polybutadiene elastomer

    Leonardo F. V. dos Santos

    2011-01-01

    Full Text Available O ZNIBU, acelerador de caráter lento foi avaliado neste trabalho em composições de polibutadieno. Este acelerador foi sintetizado com o objetivo de substituir, ou reduzir, o uso de alguns aceleradores comerciais muito utilizados em composições elastoméricas mas que, por serem formadores de nitrosaminas, podem ser prejudiciais à saúde. A fim de corrigir o caráter de acelerador lento do ZNIBU, este composto foi utilizado em conjunto com o acelerador comercial CBS (N-ciclohexil-2-benzotiazol-2-sulfenamida. Foi observado que pequenas quantidades dos dois aceleradores não são efetivas na aceleração da vulcanização nas composições do tipo goma pura. No entanto a presença de negro de fumo exerce um efeito positivo sobre a velocidade. As propriedades mecânicas estudadas mostram que o ZNIBU aumenta a resistência à tração da goma pura (35%, em comparação com a composição similar vulcanizada com CBS e, na presença do negro de fumo, este aumento é ainda mais expressivo (175%. Quanto à resistência ao rasgamento, a vulcanização com o ZNIBU forneceu o mais baixo valor da propriedade para a goma pura, enquanto que a composição com negro de fumo apresentou o mais alto valor.ZNIBU, a slow accelerator, was evaluated in polybutadiene compositions. This accelerator was synthesized intending to replace or reduce the use of some very used commercial accelerators in rubber compositions which, due to their nitrosamine-forming potential, can be harmful to health. In order to correct for the slow accelerating character ZNIBU was used in combination with the commercial accelerator CBS (N-cyclohexyl-2-benzothiazole-2-sulfenamide. It was observed that small amounts of the accelerators are not effective in the vulcanization accelerating process of gum type compositions. Nevertheless, the presence of carbon black exerts a positive effect on the reaction rate. The investigated mechanical properties show that ZNIBU improves stress strength of

  19. Graduación de datos de mortalidad y modelos lineales generalizados

    Francisco Montes Suay

    2002-01-01

    Full Text Available El objetivo de este trabajo es graduar los datos de mortalidad de la Comunidad Valenciana de 1998, mediante el ajuste de las funciones Gompertz-Makeham, GM(r,s, método utilizado por el CMI Bureau. Cuando las funciones GM(r,s carecen de la parte polinómica, r=0, la transformación logit de qx, probabilidad de muerte, puede ajustarse utilizando el esquema de los modelos lineales generalizados de fácil implementación en S-plus. En el trabajo que presentamos, hemos estimado los parámetros de funciones GM(0,s para s=2,3,4,5,6,7. La elección del modelo que mejor se ajusta a los datos se lleva a cabo atendiendo a criterios de bondad de ajuste y de complejidad del mismo. Se trata de buscar un equilibrio entre ambos aspectos, para lo cual utilizamos medidas y contrastes implementados en S-plus. Del análisis de los resultados se deduce que s=5 es el modelo que mejor satisface ambos criterios para la población masculina y s=6 para la femenina. De estos modelos hacemos un análisis más detallado mediante los tests no paramétricos habituales.

  20. Polarización lineal en estrellas simbióticas

    Brandi, E.; García, L. G.; Ferrer, O. E.

    Se presenta un estudio de polarización lineal en las bandas UBVRI de un grupo de estrellas simbióticas, a fin de analizar el comportamiento del grado de polarización y del ángulo de posición en función de la longitud de onda. En aquellos sistemas observados repetidas veces, se analizan además variaciones temporales en los parámetros de polarización. En base a este comportamiento se determina si la polarización observada es puramente interestelar o si existe una contribución de polarización, intrínseca al objeto. La muestra de objetos estudiados presenta ciertas características comunes, es decir, son sistemas simbióticos tipo D, cuyas respectivas componentes gigantes son variables tipo Mira y además presentan nebulosas ionizadas extendidas con morfología y dimensiones conocidas. Esto es de importancia ya que el conocimiento de la estructura del gas extendido permite interpretar la geometría de scattering que produce la polarización observada. Las observaciones fueron realizadas con el Fotopolarímetro de Torino adosado al telescopio de 2.15 m del CASLEO.

  1. The invention that shapes Linac4: Tolerance Aligned Cantileaver Mounting (TACM) system to build drift tube linacs

    CERN Video Productions

    2010-01-01

    Accelerator experts are no new to original 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 was indeed the case for 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.Interview with Suitbert Ramberger, Project engineer for the Linac4 Drift Tube Linac (DTL).

  2. Half wave helix loaded superconducting resonator for heavy ion Linac

    We report here the main characteristics and performances of the helix superconducting resonators designed and mounted in the new Saclay Booster Linac which is the first european heavy ion superconducting accelerator

  3. CAS CERN Accelerator School: Cyclotrons, linacs and their applications. Proceedings

    These proceedings present the lectures given at the eighth specialized course organized by the CERN Accelerator School (CAS), the topic this time being 'Cyclotrons, Linacs and Their Applications'. Following an introductory lecture on linacs, the fundamental features of electron, ion and induction linacs are described together with their RF systems and particle sources. Cyclotrons are then introduced followed by details of their different types, their magnet and RF design, and their injection and extraction systems, with a glance towards exotic and possible future machines. Chapters are then presented on the use of linacs and cyclotrons for medical, fission, fusion and material applications, as well as for isotope production. Finally, descriptions of the design of a radioisotope facility, the matching of accelerators to their task and the computational tools used in their design are included. (orig.)

  4. Ion induction linacs: reference design and proposed test-bed

    The LBL HIF program has concentrated on the induction linac approach because this type of machine is able to accelerate the entire charge required for fusion in a single, high current bunch, and because of our experience ten years ago using the Astron induction linac at LLL and subsequently building and operating our own machine at LBL. The operation of an rf linac with storage rings is based on an operating line where, excluding the tree of linacs at the lowest energies, acceleration is along a constant current trajectory to peak energy, and then along a constant energy trajectory as the current is compressed and multiplied to reach the required of beam power (> 100 TW). The operation of the linear induction accelerator is along a trajectory where the energy and current are increased simultaneously; at the end of acceleration the beam is split transversely into two groups of beams to provide for higher peak power and a left-right symmetrical pellet bombardment

  5. Error and tolerance studies for the SSC Linac

    This paper summarizes error and tolerance studies for the SSC Linac. These studies also include higher-order multipoles. The codes used in these simulations are PARMTEQ, PARMILA, CCLDYN, PARTRACE, and CCLTRACE

  6. Bunch Shape Monitors For The Desy H-Minus Linac

    Feschenko, A. V.; Liiou, A. V.; Mirzojan, A. N.; Menshov, A. A.; Ostroumov, P. N.; Holtkamp, N.; Nagl, M.; Peperkorn, I.

    1997-05-01

    In order to tune and control the longitudinal bunch shape and energy spread in the DESY Proton linac (LINAC III), three Bunch Shape Monitors (BSM) have been developed and installed. The mechanical layout has been optimised in order to fit the extremely narrow space between the DTL tanks. One of the BSMs, as an additional feature, can measure the absolute energy of the beam and is installed downstream of three Alvarez tanks. Using of thin wire as a source of secondary electrons, these devices can be used as a non-destructive beam diagnostic tool during Linac operation. The performance of the BSMs as well as the results of the Linac III studies using the new devices will be presented.

  7. Present status of the TOHOKU 300 MeV linac

    The TOHOKU linac that was constructed about a quarter century before has been operated without serious trouble recently. This report describes as follows: main trouble, maintenance, present performance of the machine and status of operation. (author)

  8. Finite element thermal study of the Linac4 plasma generator

    The temperature distribution and heat flow at equilibrium of the plasma generator of the rf-powered noncesiated Linac4 H- ion source have been studied with a finite element model. It is shown that the equilibrium temperatures obtained in the Linac4 nominal operation mode (100 kW rf power, 2 Hz repetition rate, and 0.4 ms pulse duration) are within material specifications except for the magnet cage, where a redesign may be necessary. To assess the upgrade of the Linac4 source for operation in the high-power operation mode of the Superconducting Proton Linac (SPL), an extrapolation of the heat load toward 100 kW rf power, 50 Hz repetition rate, and 0.4 ms pulse duration has been performed. The results indicate that a significant improvement of the source cooling is required to allow for operation in the high-power mode of SPL.

  9. Photonuclear reactions with Zinc: A case for clinical linacs

    Boztosun, I; Karakoç, M; Özmen, S F; Çeçen, Y; Çoban, A; Caner, T; Bayram, E; Saito, T R; Akdoğan, T; Bozkurt, V; Kuçuk, Y; Kaya, D; Harakeh, M N

    2015-01-01

    The use of bremsstrahlung photons produced by a linac to induce photonuclear reactions is wide spread. However, using a clinical linac to produce the photons is a new concept. We aimed to induce photonuclear reactions on zinc isotopes and measure the subsequent transition energies and half-lives. For this purpose, a bremsstrahlung photon beam of 18 MeV endpoint energy produced by the Philips SLI-25 linac has been used. The subsequent decay has been measured with a well-shielded single HPGe detector. The results obtained for transition energies are in good agreement with the literature data and in many cases surpass these in accuracy. For the half-lives, we are in agreement with the literature data, but do not achieve their precision. The obtained accuracy for the transition energies show what is achievable in an experiment such as ours. We demonstrate the usefulness and benefits of employing clinical linacs for nuclear physics experiments.

  10. A Radiation shielding study for the Fermilab Linac

    Rakhno, I.; Johnstone, C.; /Fermilab

    2006-02-01

    Radiation shielding calculations are performed for the Fermilab Linac enclosure and gallery. The predicted dose rates around the access labyrinth at normal operation and a comparison to measured dose rates are presented. An accident scenario is considered as well.

  11. Commissioning of the LCLS Linac and Bunch Compressors

    The Linac Coherent Light Source (LCLS) is a SASE x-ray Free-Electron Laser (FEL) project under construction at SLAC [1]. The injector section, from drive-laser and RF photocathode gun through the first bunch compressor, was commissioned in the spring and summer of 2007. The second phase of commissioning, including the second bunch compressor and various main linac modifications, was completed in January through August of 2008. We report here on experience gained during this second phase of machine commissioning, including the injector, the first and second bunch compressor stages, the linac up to 14 GeV, and beam stability measurements. The final commissioning phase, including the undulator and the long transport line from the linac, is set to begin in December 2008, with first light expected in July 2009

  12. Intraoperative radiotherapy in the theatre room with electron beams: technical and dosimetric description of Sordina LIAC accelerator; Radioterapia intraoperatoria en quirofano con haces de electrones: descripcion tecnica y dosimetrica del acelerador dedicado Sordina LIAC

    Sendon del Rio, J. R.; Ayala Lazaro, R.; Gomez Cores, S.; Garcia Hernandez, M. J.; Polo Cezon, R.; Jimenez Rojas, R.; Lopez Bote, M. A.

    2015-05-01

    n this work we show our experience during the commissioning of a mobile electron-beam accelerator dedicated to intraoperative radiation therapy in the theatre room. The linac is a Sordina LIAC 12 MeV model with a hard-docking applicator system. We describe the linac, the measurement methods and the specific dosimetry. The dosimetric behavior is also discussed. Differences with other applicator systems can be explained from the particular head design of the linac. (Author)

  13. Evolution of the 400 MeV linac design

    MacLachlan, J.A.

    1987-11-09

    The basic premises of the conceptual design for the linac upgrade are pursued to establish lengths, gradients, power dissipation, etc., for the 400 MeV linac and matching section. The discussion is limited to accelerating and focusing components. Wherever values depend on the choice of the accelerating structure, the disk-and-washer structure is emphasized; the results are generally relevant to the side coupled cavity choice also.

  14. Post-accelerator LINAC design for the VECC RIB project

    Arup Bandyopadhyay

    2002-12-01

    Variable Energy Cyclotron Centre (VECC) is presently developing an ISOL post-acclerator type of RIB facility. The scheme utilises the existing = 130 room temperature variable energy cyclotron machine as the primary accelerator for the production of RIBs and radio frequency quadrupole (RFQ) and LINAC modules for the post-acceleration. The design aspects of these postaccelerator LINAC modules will be discussed in this paper.

  15. Maintenance of KURRI-LINAC in 20 years

    KURRI-LINAC (electron linear accelerator of the Research Reactor Institute, Kyoto University) is a facility for joint use program among universities and research institutes. It was constructed in 1965. Since 1966, this facility has been used by KURRI researchers, and many joint research programs have been started in 1968. In the present report the outline of the maintenance experience of KURRI-LINAC in 20 years are described. (author)

  16. A bunch extension monitor for the SPIRAL2 LINAC

    Vignet, J.L.; Revenko, R.

    2014-01-01

    Measurements of the bunch longitudinal shape of beamparticles are crucial for optimization and control ofLINAC beam parameters and maximization of itsintegrated luminosity. The non-interceptive bunchextension monitor for the LINAC of SPIRAL2 facility isbeing developed at GANIL. Five bunch extensionmonitors will be installed at the beginning of the LINACbetween superconducting cavities. The principle ofoperation is based on the registration of x-rays induced byions of accelerator beam interact...

  17. Status report on the Saclay Heavy Ion Superconducting Linac

    The Saclay Heavy Ion Superconducting Linac is now in full operation with all 50 resonators and delivers routinely beams to Nuclear and Solid State Physics experiments since March 1989. After describing the LINAC, we give informations on the upgrading of the cryogenic system and summarize our experience of resonator behaviour on the accelerating line. Cooldown, multipactor barrier conditioning, and field raising procedures are also discussed. (author)

  18. The SSC Linac: Status of design and procurement activities

    The Linear Accelerator (Linac) is the first element in the injector chain for the Superconducting Super Collider (SSC). It must be operational by October 1995 in order to commission the Low Energy Booster (LEB). The physics design of the Linac is now essentially complete, detailed engineering is well advanced, and manufacturing has begun. This paper will review the physics design with emphasis on recent significant improvements, summarize mechanical design and construction status, and describe recent achievements in the development program

  19. The SSC linac: Status of design and procurement activities

    The Linear Accelerator (Linac) is the first clement in the injector chain for the Superconducting Super Collider (SSC). It must bc operational by October 1995 in order to commission the Low Energy Booster (LEB). The physics design of the Linac is now essentially complete, detailed engineering is well advanced, and manufacturing has begun. This paper will review the physics design with emphasis on recent significant improvements, summarize mechanical design and construction status, and describe recent achievements in the development program

  20. Measured resolutions of the Arc and Linac BPM systems

    The 6'' long final focus beam position monitors (short FF BPM's are longer, thus deliver more signal after a 15 nanosecond filter, than either the Linac or Arc monitors. The purpose of this note is to compare the resolution of the Arc vs Linac electronics when applied to a short FF 2'' diameter BPM. A method of calibrating the Arc modules is also tested and briefly discussed. The range of each DAC setting to minimize digitization error is also calculated

  1. High energy accelerating structures for high gradient proton linac applications

    The high-energy part of a proton linac, following a drift tube section, accelerates protons and H- ions of energies above 150 MeV. High efficiency and high gradients in the accelerating structure considered for this part of a proton linac are studied. Several known and improved structures working at 1350 MHz were optimized for maximum shunt impedance. The study was performed with the extensive use of a computer code--SUPERFISH. The theoretical results of this study are presented

  2. Linac 1 in the process of being pulled back

    Photographic Service

    1985-01-01

    As injector to the PS Booster, Linac 1 was replaced by Linac 2 in 1980. It continued to be used for the acceleration of oxygen and sulfur ions and, from 1981 to 1996, of protons and negative hydrogen ions for LEAR. In 1984, its Cockcroft-Walton preinjector was replaced by a much smaller RFQ, which allowed it to be moved to a more convenient location.

  3. Acceleration test of heavy ion RFQ linac at TIT

    An 80 MHz heavy ion RFQ linac at Tokyo Institute of Technology (TIT) has been constructed for research on inertial fusion and plasma experiments. Equipment for beam acceleration has been fabricated and assembled to confirm the performance with low currents of the RFQ. The linac successfully accelerated He+ and C2+ ion beams to their final energies of 219 keV/u. The obtained beam transmission was more than 89% with currents of a few tens μA. (orig.)

  4. Trends in Intermediate-Energy Superconducting wide-β Linacs

    Superconducting low beta linacs have been developed during the last 20 years as heavy ion accelerators for nuclear research; such linacs, mainly made of 2 or 3 gap superconducting cavities, are used in many countries as boosters for tandem accelerators and also as standalone machines. An important contribution in this field was given by the Weizmann Institute, where the first superconducting quarter wave booster was developed, becoming the model for many other machines around the world

  5. Effect of cooling water on stability of NLC linac components

    F. Le Pimpec et al.

    2003-02-11

    Vertical vibration of linac components (accelerating structures, girders and quadrupoles) in the NLC has been studied experimentally and analytically. Effects such as structural resonances and vibration caused by cooling water both in accelerating structures and quadrupoles have been considered. Experimental data has been compared with analytical predictions and simulations using ANSYS. A design, incorporating the proper decoupling of structure vibrations from the linac quadrupoles, is being pursued.

  6. Physics design of APT linac with normal conducting rf cavities

    The accelerator based production of tritium calls for a high-power, cw proton linac. Previous designs for such a linac use a radiofrequency quadrupole (RFQ), followed by a drift-tube linac (DTL) to an intermediate energy and a coupled-cavity linc (CCL) to the final energy. The Los Alamos design uses a high-energy (6.7 MeV) RFQ followed by the newly developed coupled-cavity drift-tube linac (CCDTL) and a CCL. This design accommodates external electromagnetic quadrupole lenses which provide a strong uniform focusing lattice from the end of the RFQ to the end of the CCL. The cell lengths in linacs of traditional design are typically graded as a function of particle velocity. By making groups of cells symmetric in both the CCDTL and CCL, the cavity design as well as mechanical design and fabrication is simplified without compromising the performance. At higher energies, there are some advantages of using superconducting rf cavities. Currently, such schemes are under vigorous study. This paper describes the linac design based on normal conducting cavities and presents simulation results

  7. The 400 MeV Linac Upgrade at Fermilab

    Noble, R.J.

    1992-12-01

    The Fermilab Linac Upgrade in planned to increase the energy of the H{sup {minus}} linac from 200 to 400 MeV. This is intended to reduce the incoherent space-charge tuneshift at injection into the 8 GeV Booster which limit either the brightness or the total intensity of the beam. The Linac Upgrade will be achieved by replacing the last four 201.25 MHs drift-tube linac (DTL) tanks which accelerate the beam from 116 to 200 MeV, with seven 805 MRs side-coupled cavity modules operating at an average axial field of about 7.5 MV/meter. This will allow acceleration to 400 MeV in the existing Linac enclosure. Each accelerator module will be driven with a 12 MW klystron-based rf power supply. Three of seven accelerator modules have been fabricated, power tested and installed in their temporary location adjacent to the existing DTL. All seven RF Modulators have been completed and klystron installation has begun. Waveguide runs have completed from the power supply gallery to the accelerator modules. The new linac will be powered in the temporary position without beam in order to verify overall system reliability until the laboratory operating schedule permits final conversion to 400 MeV operation.

  8. Status and plans for Linac4 installation and commissioning

    Vretenar, M; Arnaudon, L; Baudrenghien, P; Bellodi, G; Broere, J; Brunner, O; Comblin, J F; Coupard, J; Dimov, V A; Fuchs, J F; Funken, A; Gerigk, F; Granemann Souza, E; Hanke, K; Hansen, J; Yarmohammadi Satri, M; Kozsar, I; Lallement, J B; Lenardon, F; Lettry, J; Lombardi, A M; Maglioni, C; Midtun, O; Mikulec, B; Nisbet, D; Paoluzzi, M; Raich, U; Ramberger, S; Roncarolo, F; Rossi, C; Sanchez Alvarez, J L; Scrivens, R; Tan, J; Valerio-Lizarraga, C A; Vollaire, J; Wegner, R; Weisz, S; Zocca, F

    2014-01-01

    Linac4 is a normal conducting 160 MeV Hˉ linear accelerator presently being installed and progressively commissioned at CERN. It will replace the ageing 50 MeV Linac2 as injector of the PS Booster (PSB), increasing at the same time its brightness by a factor of two thanks to the higher injection energy. This will be the first step of a program to increase the beam brightness in the LHC injectors for the needs of the High-Luminosity LHC project. After a series of beam measurements on a dedicated test stand the 3 MeV Linac4 front-end, including ion source, RFQ and a beam chopping line, has been recommissioned at its final position in the Linac4 tunnel. Commissioning of the following section, the Drift Tube Linac, is starting. Beam commissioning will take place in steps of increasing energy, to reach the final 160 MeV in 2015. An extended beam measurement phase including testing of stripping equipment for the PSB and a year-long test run to assess and improve Linac4 reliability will take place in 2016, prior to...

  9. Progress in the Construction of Linac4 at CERN

    Vretenar, M; Baudrenghien, P; Bertone, C; Body, Y; Broere, J; Brunner, O; Bellodi, G; Buzio, M; Carli, C; Roncarolo, F; Ramberger, S; Raich, U; Puccio, B; Paoluzzi, M; Nisbet, D; Mikulec, B; Mathot, S; Maglioni, C; Lopez-Hernandez, LA; Lombardi, A; Lallement, J B; Lettry, J; Kozsar, I; Hansen, J; Hanke, K; Hammouti, L; Gerigk, F; Garoby, R; Funken, A; Fuchs, J F; Dos Santos, N; Dallocchio, A; Coupard, J; Corso, JP; Scrivens, R; Schwerg, N; Vollaire, J; Zickler, T; Weisz, S; Wegner, R; Vandoni, G; Rossi, C

    2013-01-01

    As first step of the LHC luminosity upgrade program CERN is building a new 160 MeV H¯ linear accelerator, Linac4, to replace the ageing 50 MeV Linac2 as injector to the PS Booster (PSB). Linac4 is an 86-m long normalconducting linac made of a 3 MeV injector followed by 22 accelerating cavities of three different types. The general service infrastructure has been installed in the new tunnel and surface building and its commissioning is progressing; high power RF equipment is being installed in the hall and installations in the tunnel will start soon. Construction of the accelerator parts is in full swing involving industry, the CERN workshops and a network of international collaborations. The injector section including a newly designed and built H¯ source, a 3-m long RFQ and a chopping line is being commissioned in a dedicated test stand. Beam commissioning of the linac will take place in steps of increasing energy between 2013 and 2015. From end of 2014 Linac4 could deliver 50 MeV protons i...

  10. Linac design for intense hadron beams

    Zhang, Chuan

    2009-12-14

    Based on the RFQ and H-type DTL structures, this dissertation is dedicated to study the beam dynamics in the presence of significantly strong space-charge effects while accelerating intense hadron beams in the low- and medium-{beta} region. Besides the 5 mA/30 mA, 17 MeV proton injector (RFQ+DTL) and the 125 mA, 40 MeV deuteron DTL of the EUROTRANS and IFMIF facilities, a 200 mA, 700 keV proton RFQ has been also intensively studied for a small-scale but ultra-intense neutron source FRANZ planned at Frankfurt University. The most remarkable properties of the FRANZ RFQ and the IFMIF DTL are the design beam intensities, 200 mA and 125 mA. A new design approach, which can provide a balanced and accelerated beam bunching at low energy, has been developed for intense beams. To design the IFMIF DTL and the injector DTL part of the EUROTRANS driver linac, which have been foreseen as the first real applications of the novel superconducting CH-DTL structure, intensive attempts have been made to fulfill the design goals under the new conditions. For the IFMIF DTL, the preliminary IAP design has been considerably improved with respect to the linac layout as well as the beam dynamics. By reserving sufficient drift spaces for the cryosystem, diagnostic devices, tuner and steerer, introducing SC solenoid lenses and adjusting the accelerating gradients and accordingly other configurations of the cavities, a more realistic, reliable and efficient linac system has been designed. On the other hand, the specifications and positions of the transverse focusing elements as well as the phase- and energy-differences between the bunch-center particle and the synchronous particle at the beginning of the {phi}{sub s}=0 sections have been totally redesigned. For the EUROTRANS injector DTL, in addition to the above-mentioned procedures, extra optimization concepts to coordinate the beam dynamics between two intensities have been applied. In the beam transport simulations for both DTL designs

  11. Linac design for intense hadron beams

    Based on the RFQ and H-type DTL structures, this dissertation is dedicated to study the beam dynamics in the presence of significantly strong space-charge effects while accelerating intense hadron beams in the low- and medium-β region. Besides the 5 mA/30 mA, 17 MeV proton injector (RFQ+DTL) and the 125 mA, 40 MeV deuteron DTL of the EUROTRANS and IFMIF facilities, a 200 mA, 700 keV proton RFQ has been also intensively studied for a small-scale but ultra-intense neutron source FRANZ planned at Frankfurt University. The most remarkable properties of the FRANZ RFQ and the IFMIF DTL are the design beam intensities, 200 mA and 125 mA. A new design approach, which can provide a balanced and accelerated beam bunching at low energy, has been developed for intense beams. To design the IFMIF DTL and the injector DTL part of the EUROTRANS driver linac, which have been foreseen as the first real applications of the novel superconducting CH-DTL structure, intensive attempts have been made to fulfill the design goals under the new conditions. For the IFMIF DTL, the preliminary IAP design has been considerably improved with respect to the linac layout as well as the beam dynamics. By reserving sufficient drift spaces for the cryosystem, diagnostic devices, tuner and steerer, introducing SC solenoid lenses and adjusting the accelerating gradients and accordingly other configurations of the cavities, a more realistic, reliable and efficient linac system has been designed. On the other hand, the specifications and positions of the transverse focusing elements as well as the phase- and energy-differences between the bunch-center particle and the synchronous particle at the beginning of the φs=0 sections have been totally redesigned. For the EUROTRANS injector DTL, in addition to the above-mentioned procedures, extra optimization concepts to coordinate the beam dynamics between two intensities have been applied. In the beam transport simulations for both DTL designs, no beam losses

  12. Klystron power supply systems for J-PARC linac. Report of construction status and 60MeV linac operation

    The Accelerators for the High Intensity Proton Accelerator Facility Project (J-PARC) are now under construction in the Tokai area. The klystron power supply systems for the J-PARC Linac have been installing since this April. This paper reports the construction status of the systems, and the operation of the systems for the 60MeV Linac in the Tsukuba area. (author)

  13. Dose reduction using non lineal diffusion and smoothing filters in computed radiography

    The use of Computed Radiography (CR) into clinical practice has been followed by a high increase in the number of examinations performed and overdose cases in patients, especially children in pediatric applications. Computed radiographic images are corrupted by noise because either data acquisition or data transmission. The level of this inherent noise is related with the X-ray dose exposure: lower radiation exposure involves higher noise level. The main aim of this work is to reduce the noise present in a low radiation dose CR image in order to the get a CR image of the same quality as a higher radiation exposure image. In this work, we use a non lineal diffusion filtering method to reduce the noise level in a CR, this means that we are able to reduce the exposure, milliampere-second (mAs), and the dose absorbed by the patients. In order to get an optimal result, the diffusive filter is complemented with a smoothing filter with edge detection in order to preserve edges. Therefore, the proposed method consists in obtaining a good quality CR image for diagnostic purposes by selection of lower X-ray exposure jointly with a reduction of the noise. We conclude that a good solution to minimize the dose to patients, especially children in pediatric applications, in X-ray computed radiography consists in decreasing the mAs of the X-ray exposure and then processing the image with the proposed method. - Highlights: • We have investigated the techniques to obtain the image quality to make a confident diagnosis. • We have used diffusion and smoothing filter in order to reduce the exposure. • Reducing CR doses, especially in pediatric applications. • The new CR images allow medical researchers to analyze how low dose affects the patient diagnosis

  14. Study of space charge-dominated beam bunching and some aspects of SSF linac designs

    This report is made up from works under the Agreement 1083P0015-35 between Los Alamos National Laboratory and Moscow Radiotechnical Institute. There are five report parts. In the 1-st, 2-nd, and 3-d parts works on SCD-beam dynamics understanding were continued. In the 4-th and 5-th parts two conceptual linac designs were considered: for deutron linac with energy of 40 MeV and for proton linac with energy 1 GeV. The both linacs have focusing by superconducting solenoids (SSF linacs). The 1 GeV proton CW linac design is an extension of the design from

  15. Linac4 chopper line commissioning strategy

    Bellodi, G; Lombardi, A M; Posocco, P A; Sargsyan, E

    2010-01-01

    The report outlines the strategy for beam-based commissioning of the Linac4 3 MeV chopper line as currently scheduled to start in the second half of 2011 in the Test Stand Area. A dedicated temporary diagnostics test bench will complement the measurement devices foreseen for permanent installation in the chopper line. A commissioning procedure is set out as a series of consecutive phases, each one supposed to meet a well- defined milestone in the path to fully characterise the beam-line. Specific set-ups for each stage are defined in terms of beam characteristics, machine settings and diagnostics used. Operational guidelines are given and expected results at the relative points of measurements are shown for simulated scenarios (on the basis of multi-particle tracking studies carried out with the codes PATH and TRACEWin). These are then interpreted in the light of the resolution limits of the available diagnostics instruments to assess the precision reach on individual measurements and the feasibility of techn...

  16. Bunching system of the KEKB linac

    At present, the KEK 2.5-GeV Linac is being upgraded as the injector of the KEK B-factory (KEKB). One of the most important changes is to increase the intensities of positron beams injected into a KEKB ring; it is, therefore, required to accelerate high-intensity single-bunch electron beams to high energy, 3.7 GeV, where they are converted to positron beams. For the purpose, the primary electron bunch should have more than 10 nC. Furthermore, the bunch lengths must be limited as short as 10 ps, in order to achieve narrow energy spreads of primary electron beams, and produce positron beams of short bunch lengths, as well. The bunching system has been designed to meet these requirements, introducing subharmonic bunchers (SHB). This paper describes the upgrade of the bunching system and the results of simulations of bunching using PARMELA. The designs and RF test of SHB cavities are described. (author)

  17. Development of head docking device for linac-based radiosurgery with a Neptun 10 PC linac.

    Khoshbin Khoshnazar, Alireza; Bahreyni Toossi, Mohammad Taghi; Hashemian, Abdolreza; Salek, Roham

    Stereotactic radiosurgery is a method for focused irradiation of intracranial lesions. Linac-based radiosurgery is currently performed by two techniques: couch mounted and pedestal mounted. In the first technique a device is required to affix the patient's head to the couch and neoreover to translate it accurately. Structure of such a device constructed by the authors plus acceptance test performed for evaluation is described in the article. A head docking device has been designed and constructed according to geometry of linac's couch and also desired functions. The device is cornpletely made from aluminum and consists of four major components: attachment bar, lower structure with four moveing accuracy mechanical stability and isocentric accuracy were assessed in the frame of acceptance test. Translating accuracy, mechanical stability and isocentric accuracy were found to be respectively: 1 mm, 1.64 mm and 3.2 mm with accuracy of 95%. According to AAPM report no. 54, a head docking device should translate head with an accuracy of 1 mm; this recommendation has been met. Moreover, we have demonstrated that the isocentric accuracy and mechanical stability of the device are sufficient that the device on confidently be used in stereotactic treatment. PMID:17664152

  18. Fermilab 200 MeV linac control system hardware

    This report is a description of the present Linac distributed control system that replaces the original Xerox computer and interface electronics with a network of 68000-based stations. In addition to replacing the obsolete Xerox equipment, goals set for the new system were to retain the fast response and interactive nature of the original system, to improve reliability, to ease maintenance, and to provide 15 Hz monitoring of all Linac parameters. Our previous experience with microcomputer installations showed that small, stand-alone control systems are rather straightforward to implement and have been proven to be reliable in operation, even in the severe environment of the 750-keV preaccelerator. The overall design of the Linac system incorporates the concept of many relatively small, stand-alone control systems networked together using an intercomputer communication network. Each station retains its local control system character but takes advantage of the network to allow an operator to interact with the entire Linac from any local console. At the same time, a link to the central computer system allows Host computers to also access parameters in the Linac

  19. Fermilab 200 MeV linac control system hardware

    Shea, M.F.

    1984-01-01

    This report is a description of the present Linac distributed control system that replaces the original Xerox computer and interface electronics with a network of 68000-based stations. In addition to replacing the obsolete Xerox equipment, goals set for the new system were to retain the fast response and interactive nature of the original system, to improve reliability, to ease maintenance, and to provide 15 Hz monitoring of all Linac parameters. Our previous experience with microcomputer installations showed that small, stand-alone control systems are rather straightforward to implement and have been proven to be reliable in operation, even in the severe environment of the 750-keV preaccelerator. The overall design of the Linac system incorporates the concept of many relatively small, stand-alone control systems networked together using an intercomputer communication network. Each station retains its local control system character but takes advantage of the network to allow an operator to interact with the entire Linac from any local console. At the same time, a link to the central computer system allows Host computers to also access parameters in the Linac.

  20. Mechanical Engineering of the Linac for the Spallation Neutron Source

    The linac for the Spallation Neutron Source (SNS) Project will accelerate an average current of 1 mA of H- ions from 20 MeV to 1GeV for injection into an accumulator ring. The linac will be an intense source of H- ions and as such requires advanced design techniques to meet project technical goals as well as to minimize costs. The DTL, CCDTL and CCL are 466m long and operate at 805 MHz with a maximum H- input current of 28 mA and 7% rf duty factor. The Drift Tube Linac is a copper-plated steel structure using permanent magnetic quadrupoles. The Coupled-Cavity portions are brazed copper structures and use electromagnetic quads. RF losses in the copper are 80 MW, with total rf power supplied by 52 klystrons. Additionally, the linac is to be upgraded to the 2- and 4-MW beam power levels with no increase in duty factor. The authors give an overview of the linac mechanical engineering effort and discuss the special challenges and status of the effort

  1. Higher order beam jitter in the SLC linac

    The pulse-to-pulse behavior of the beams in the SLC linac is dominated by wakefields which can amplify any other sources of jitter. A strong focusing lattice combined with BNS damping controls the amplitude of oscillations which otherwise would grow exponentially. Measurements of oscillation amplitude along the linac show beam motion that is up to six times larger than that expected from injection jitter. A search for possible sources of jitter within the linac uncovered some problems such as structure jitter at 8 to 12 Hz, pump vibrations at 59 Hz and 1 Hz aliasing by the feedback systems. These account for only a small fraction of the observed jitter which is dominantly white noise. No source has yet been fully identified but possible candidates are dark current in the linac structures (not confirmed by experiment) or subtle correlations in injection jitter. An example would be a correlated x-z jitter with no net offset visible on the beam position monitors at injection. Such a correlation would cause jitter growth along the linac as wakefields from the head of the bunch deflect the core and tail of the bunch. Estimates of the magnitude of this effect and some possible sources are discussed in this paper. (author)

  2. A heavy ion linac complex for unstable nuclei

    A heavy ion linac complex for unstable nuclei is under construction at INS. The linac complex consists of a 25.5-MHz split coaxial RFQ (SCRFQ), a charge-stripper section, and a 51-MHz interdigital-H (IH) linac. The SCRFQ with modulated vanes, 0.9 m in diameter and 8.6 m in length, accelerates ions with a charge-to-mass ratio (q/A) greater than 1/30 from 2 to 170 keV/u. The stripper is a carbon foil. The IH linac, 1.34 m in diameter and 5.54 m in total length, comprises four cavities and three magnetic quadrupole triplets placed between cavities, accelerates ions with q/A ≥ 1/10, and varies the output energy continuously in the range 0.17 - 1.05 MeV/u. The duty factor of the linac complex is 30% for q/A = 1/30 ions. (author)

  3. CERN Linac4 - The Space Charge Challenge Design and Commission

    Hein, Lutz Matthias; Holzer, Bernhard

    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 re-construct 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...

  4. Proceedings of the workshop on 'radiation protection in LINACs'

    The proceedings contain seven reports on electron and proton accelerators currently used in Japan. The first report describes the 'Present Condition of Linac Facilities in Japan -- Questionnaire Survey'. It summarizes results of a questionnaire survey on 400 facilities where accelerators are used for research, industrial or medical applications. The second one deals with 'Radiation Protection at Nuclear Physics Research Institute of Tohoku University'. Safety measures taken in the institute are described. The third report outlines 'Radiation Protection at Linac Facility in Tokai Laboratory of Japan Atomic Energy Research Institute, focusing on equipment, radiation management, and safety measures. The fourth report, titled 'Proton Linac at High Energy Physics Research Institute', outlines major features of the facilities in the institute, radiation safety measures, etc. The fifth one describes the 'Safety Management at Electrotechnical Laboratory', centering on the equipment used, radiation management, and safety measures. The sixth one outlines major features of 'Electron Linac at Industrial Science Research Institute of Osaka University'. The seventh report describes the 'Present Condition of Neutron Generator (KURRI-LINAC)'. (N.K.)

  5. Heavy-ion LINAC development for the US RIA project

    P N Ostroumov

    2002-12-01

    The Nuclear Science Community in the Unites States has unanimously concluded that developments in both nuclear science and its supporting technologies make building a world-leading Rare-Isotope Accelerator (RIA) facility for production of radioactive beams the top priority. The RIA development effort involves several US Laboratories (ANL, JLAB, LBNL, MSU, ORNL). The RIA facility includes a CW 1.4 GeV driver LINAC and a 100 MV post-accelerator both based on superconducting (SC) cavities operating at frequencies from 48 MHz to 805 MHz. An initial acceleration in both LINACs is provided by room temperature RFQs. The driver LINAC is designed for acceleration of any ion species; from protons up to 900 MeV to uranium up to 400 MeV/u. The novel feature of the driver LINAC is an acceleration of multiple charge-state heavy-ion beams in order to achieve 400 kW beam power. Basic design concepts of the driver LINAC are given. Several new conceptual solutions in beam dynamics, room temperature and SC accelerating structures for heavy ion accelerator applications are discussed.

  6. Análisis del pandeo de pilares en régimen no lineal mediante splines generalizados

    Ortega Sánchez, Miguel Angel

    2004-01-01

    El objetivo fundamental de la presente memoria ha sido la realización de un estudio sobre el comportamiento de los pilares esbeltos sometidos a pandeo en régimen no lineal mediante la técnica de splines generalizados. Dicha técnica puede considerarse como una variante de la metodología de cálculo por elementos finitos. Para ello tras una revisión de los antecedentes históricos y los métodos actuales de cálculo de elementos viga-columna sometidos a cargas axiles en situaciones de no linealidad...

  7. Uso de la heurística “Optimización gravitatoria” con funciones no lineales

    Alegre, Jesús F.; Pacheco, Joaquín A.; Zapatero, María J.

    2009-01-01

    RESUMEN En el trabajo se propone una heurística basada en la estrategia denominada Optimización Gravitatoria, para la obtención de óptimos globales en varias funciones no lineales, algunas de ellas multimodales. En esta heurística se concibe el espacio de soluciones de forma similar al espacio-tiempo relativista, en el que la métrica es modificada por el campo gravitatorio generado por las diferentes partículas en él inmersas. En la heurística el papel de la atracción gravitatoria lo juega la...

  8. Modelación matemática en la resolución de sistemas de ecuaciones lineales

    López, Jorge Iván; Flores, Ángel

    2012-01-01

    El presente trabajo se enfoca a realizar un estudio del impacto que tiene la Modelación Matemática en el aprendizaje de sistemas de ecuaciones lineales dentro del contexto de enseñanza Aprender Matemática, Haciendo Matemática. Este modelo de enseñanza se fundamenta en el marco teórico de Vygotsky y se busca que el alumno desarrolle una Cultura Básica a partir de dos aspectos fundamentales: Competencias: las cuales comprenden: el desarrollo de un pensamiento matemático, la capacidad de resolve...

  9. Comportamiento sísmico de edificios con un sistema no lineal de control híbrido

    Barbat Barbat, Horia Alejandro; Rodellar Benedé, José; Ryan, Eugene P.; Molinares, Nelson

    1993-01-01

    En el artículo se propone una clase de sistema hi33rido de control antisísmico de edificios que combina un sistema pasivo de aislamiento de base con comportamiento no lineal con uno, activo. La componente pasiva del sistema está constituida por un aparato de apoyo que puedeser de tipo histerético, de tipo friccional, o una combinación de los dos. Las fuerzas de controlactivo se aplican sobre la base y tienen como objetivo la reducción de su desplazamiento. Se desarrolla una ley de control ada...

  10. Ayuda visual basada en un sistema electrónico de magnificación no lineal

    Romero Torres, Eva

    2011-01-01

    Este proyecto se basa en la implementación de una ayuda óptica para personas que poseen baja visión. Concretamente la ayuda que se pretende desarrollar en este trabajo es electrónica y está basada en sistemas de magnificación no lineal. Este tipo de magnificación electrónica no existe comercialmente. Por esta razón se ha decido realizar este proyecto fin de carrera y por ello es necesaria la realización de ensayos clínicos posteriores con pacientes para poder verificar su utilidad. Cada uno d...

  11. Análisis no lineal de sistemas de control de nivel con algoritmo exponencial polinómico

    Posada Jaramillo, Ricardo; Navarro Betancur, Guillermo Adolfo

    2010-01-01

    El objetivo de este trabajo es el análisis de las características no lineales en un sistema de control de nivel mediante el algoritmo exponencial polinómico propuesto por J. P. Shunta. El nivel del fluido en el recipiente -el cual está manipulado por una válvula- debe mantenerse en un valor promedio determinado -- De acuerdo con los medios utilizados, el trabajo fue del tipo documental y computacional. Se aplicaron definiciones y teoremas del análisis matemático y de la teoría de control no ...

  12. Pronóstico de la serie de Mackey-Glass Usando modelos de regresión no lineal

    Juan David Velásquez Henao

    2004-01-01

    Tres t´ecnicas de regresi´on no lineal son estudiadas y se compara su desempeno en el pron´ostico de la serie de tiempo de MackeyGlass. La primera de ellas es el modelo MARS, que se plantea como una alternativa a los modelos conexionistas. El segundo es el Sistema de Inferencia Difusa Adaptativo (ANFIS), y el tercero es la red neuronal de propagaci´on hacia delante, ampliamente utilizada en aplicaciones de ingenier´ıa y econom´ıa. Los resultados muestran claramente co...

  13. Entorno web para la enseñanza del Método de Programación Lineal

    López, María Victoria; Golobisky, María F.; Mariño, Sonia Itatí

    2002-01-01

    Este trabajo tiene como objetivo el desarrollo de una aplicación Web de tipo tutorial que permitirá transmitir a los estudiantes los contenidos temáticos referentes al Método de Programación Lineal, que conforman el Programa de la cátedra Investigación Operativa de la carrera de Licenciatura en Sistemas de Información de la Facultad de Ciencias Exactas y Naturales y Agrimensura (UNNE). Se presentan los resultados consistentes en el diseño e implementación de esta herramienta. Se logró u...

  14. Estudio de los métodos de representación de diagramas espacio tiempo en obras lineales

    Artieda Monge, Tirso

    2014-01-01

    Los diagramas espacio-tiempo (DET) son una herramienta muy eficaz en la planificación en obras lineales. Sin embargo, los programas informáticos más populares en gestión de proyectos, como Primavera PG o Microsoft Project, no incluyen esta herramienta. Un análisis del software existente que ofrece este sistema en la actualidad, facilita el conocimiento sobre las diferentes opciones presentes para la incorporación de estos diagramas a la planificación de un proyecto, mejorando la calida...

  15. Regresión no lineal mediante la evolución de modelos Híbridos de Redes Neuronales

    Hervás-Martínez, César; Francisco J Martínez; Pedro A. Gutiérrez; Ruiz, Aarón

    2005-01-01

    El presente trabajo es una primera aproximación a la formación de modelos de redes neuronales con unidades ocultas de tipo híbrido (sigmoides, producto) que siendo aproximadores universales, puedan utilizarse como modelos no lineales de regresión cuando las características del espacio de las variables independientes lo aconsejen. Dada la dificultad que presenta la aplicación de algoritmos de aprendizaje de búsqueda local para esta tipología de modelos, se utiliza un...

  16. Un nuevo algoritmo para la solución de problemas de programación lineal

    Ramírez Leal, Andrés Leonardo; Buitrago Suescún, Oscar Yecid; Britto Agudelo, Rodrigo Alberto

    2012-01-01

    La programación lineal (PL) es una de las herramientas de mayor aplicación en la investigación de operaciones. Se han desarrollado y se siguen proponiendo varios métodos para la resolución de problemas de este tipo, desde el famoso simplex hasta los algoritmos de punto interior. Este trabajo tiene como propósito principal presentar la propuesta de un nuevo procedimiento para la solución de problemas PL que, partiendo de un punto interior, realiza proyecciones ortogonales mediante rectas param...

  17. Extracción de características de ecg basadas en transformaciones no lineales y wavelets

    Montes, Victoria Eugenia; Gustavo A Guarín; CASTELLANOS DOMÍNGUEZ, GERMÁN

    2010-01-01

    Se presentan diferentes métodos de extracción de caracterIsticas en senales ECG normales y en presencia de eventos relacionados con cardiopatIa isquémica, basados en mediciones de diagnóstico, la transformada wavelet y el análisis no lineal de componentes principales. Con el fin de determinar las caracterIsticas que contribuyen de melor manera con el modelo, se aplican dos técnicas de selección efectiva de caracterIsticas empleando métodos estadIsticos multivariados y univariados. La evaluaci...

  18. First successful beam test of niobium based superconducting linac at Nuclear Science Centre

    To increase the energy of the ion beam from Pelletron accelerator, a superconducting booster linear accelerator (linac) is under construction. Quarter wave resonator (QWR) made by niobium has been chosen as the accelerating unit of our Linac. Recently eight resonators along with a superconducting solenoid had been installed and aligned in the first linac cryostat. In the on-line test beam transmission through the linac was measured to be ∼100%. A pulsed beam of 28Si+7, 90 MeV, 1.5 ns FWHM was injected into the superbuncher which produced a beam of 300 ps FWHM at the entrance of linac. By turning on resonators one by one in linac cryostat and carefully adjusting their reference phases, a total energy gain of ∼ 6 MeV was measured at the exit of linac. Details of different systems of the linac and its on line beam experiment is presented in this paper. (author)

  19. Monte Carlo simulation of the Varian Clinac 600C accelerator using dynamic wedges; Simulacao Monte Carlo do acelerador Varian Clinac 600C utilizando cunhas dinamicas

    Moreno, S. [Universidade da Beira Interior (UBI), Covilha (Portugal); Chaves, A.; Lopes, M.C. [Instituto Portugues de Oncologia Doutor Francisco Gentil (IPO), Coimbra (Portugal); Peralta, L. [Laboratorio de Instrumentacao e Fisica Experimental de Particulas (LIP), Lisboa (Portugal)]|[Universidade de Lisboa (Portugal). Faculdade de Ciencias

    2004-07-01

    The advent of linear accelerators (linac) with computer-controlled dynamic collimation systems and functional and anatomical imaging techniques allowed a more exact delimitation and localisation of the target volume. These advanced treatment techniques inevitably increase the complexity level of dose calculation because of the introduction of the temporal variable. On account of this, it is mandatory the usage of more accurate modelling techniques of the collimator components, as it is the case of Monte Carlo (MC) simulation, which has created an enormous interest in research and clinical practice. Because the patients bodies are not homogenous nor are their body surfaces plane and regular, the dose distribution may differ significantly from the standard distribution from the linac calibration. It is in the treatment planning systems, which include algorithms that are usually measured in homogeneous water phantoms specific for each correction that the dose distributions from each case are obtained. In a real treatment, exception made to superficial lesions, two or more radiation fields are used in order to obtain the recommended dose distributions. The simplest arrangement is made from two parallel and opposed fields that originate a homogeneous dose distribution in almost all the irradiated volume. The available resources are, for example, different types of energies and of radiation, the application of bolus, the protection of healthy structures, the usage of wedged filters and the application of dynamic wedges. A virtual or dynamic wedge, modelled through the movement of one of the jaws, when compared with a set of physical wedges offers an alternative calculation method of an arbitrary number of wedged fields, instead of the four traditional fields of 15 deg, 30 deg, 45 deg and 60 deg angle and obtained with physical wedges. The goal of this work consists in the study of the application of dynamic wedges in tailoring the radiation field by the Varian Clinac 600

  20. Linac injector options for a relativistic heavy ion synchrotron

    A growing interest in medical uses for high energy heavy ion beams has led to two recent proposals to build dedicated medical heavy ion synchrotrons. Linear accelerators are generally preferred as injectors for synchrotrons, but in the case of heavy ions with relatively low charge to mass ratios, the required linacs are extremely large, and/or complex, low frequency structures. Cyclotrons were therefore initially proposed as the injectors for the medical synchrotrons. Recently a new radio-frequency quadrupole (RFQ) linac structure has been developed. Its excellent capture, beam transport and acceleration characteristics for low velocity ion beams makes it ideally suited as a heavy ion synchrotron injector either alone or in combination with a drift tube linac

  1. Application of RF crossed lenses for beam focusing in linac

    A method of beam focusing by two-electrode RF crossed lenses with decelerating fields is proposed. The lenses are arranged in accelerating gaps of a drift tube linac. The crossed lens is a set of plane electrodes with rectangular apertures such that the apertures in the neighbouring electrodes are rotated 90 degrees each other. Different variants of the focusing period structure are considered. The βλ FD period is shown to be used for low energy part of the linac. The transverse phase advance for the FD period is independent on the particle phase when the synchronous harmonics of the accelerating field is absent and the structure is analogous to RFQ with unmodulated vanes in the case. In the main part of the linac it is worth to change to the 2βλ FODO period to obtain essentially higher acceleration rate. (author)

  2. Status of Superconducting RF Linac Development for APT

    Chan, K C D; Gautier, D C; Gentzlinger, R C; Gioia, J G; Haynes, W B; Katonak, D J; Kelley, J P; Krawczyk, F L; Madrid, M A; Mitchell, R R; Montoya, D I; Schmierer, E N; Schrage, D L; Shapiro, A H; Tajima, T; Waynert, J A; Mammosser, J; Kuzminski, J

    2000-01-01

    This paper describes the development progress of high current superconducting RF linacs in Los Alamos, performed to support a design of the linac for the APT (Accelerator Production of Tritium) Project. The APT linac design includes a CW superconducting RF high energy section, spanning an energy range of 211 to 1030 MeV, and operating at a frequency of 700 MHz with two constant beta sections (beta of 0.64 and 0.82). In the last two years, we have progressed towards build a cryomodule with beta of 0.64. We completed the designs of the 5 cell superconducting cavities and the 210 kW power couplers. We are scheduled to begin assembly of the cryomodule in September 2000. In this paper, we present an overview of the status of our development efforts and a report on the results of the cavity and coupler test program.

  3. Investigations of Slow Motions of the SLAC Linac Tunnel

    Seryi, Andrei

    2000-01-01

    Investigations of slow transverse motion of the linac tunnel of the Stanford Linear Collider have been performed over period of about one month in December 1999 -- January 2000. The linac laser alignment system, equipped with a quadrant photodetector, allowed submicron resolution measurement of the motion of the middle of the linac tunnel with respect to its ends. Measurements revealed two major sources responsible for the observed relative motion. Variation of the external atmospheric pressure was found to be the most significant cause of short wavelength transverse motion of the tunnel. The long wavelength component of the motion has been also observed to have a large contribution from tidal effects. The measured data are essential for determination of parameters for the Next Linear Collider.

  4. Investigations of Slow Motions of the SLAC Linac Tunnel

    Investigations of slow transverse motion of the linac tunnel of the Stanford Linear Collider have been performed over period of about one month in December 1999--January 2000. The linac laser alignment system, equipped with a quadrant photodetector, allowed submicron resolution measurement of the motion of the middle of the linac tunnel with respect to its ends. Measurements revealed two major sources responsible for the observed relative motion. Variation of the external atmospheric pressure was found to be the most significant cause of short wavelength transverse motion of the tunnel. The long wavelength component of the motion has been also observed to have a large contribution from tidal effects. The measured data are essential for determination of parameters for the Next Linear Collider

  5. Collective electron driven linac for high energy physics

    A linac design is presented in which an intense ultrarelativistic electron bunch is used to excite fields in a series of cavities and accelerate charged particles. The intense electron bunch is generated in a simple storage ring to have the required transverse and longitudinal dimensions. The bunch is then transferred to the linac. The linac structure can be inexpensively constructed of spacers and washers. The fields in the cells resulting from the bunch passage are calculated using the program BCI. The results show that certain particles within the driving bunch and also trailing particles of any sign charge can be accelerated. With existing electron storage rings, accelerating gradients greater than 16 MV/m are possible. Examples of two accelerators are given: a 30 GeV electron/positron accelerator useful as an injector for a high energy storage ring and 2) a 110 GeV per beam electron-positron collider

  6. Fast alternate beam injection from SPring-8 linac

    The electron beam from SPring-8 linac has been distributed to the booster synchrotron (Sy) of SPring-8 and New SUBARU (NS) of University of Hyogo. The beam direction from the linac had been changed every fifteen or twenty seconds in TopUp operation by sending command messages to network devices from central control room. Because the commands are software-based and executed successively one by one, it took about ten seconds to complete them. To change the beam routes every 0.5 seconds, we modified the timing system of linac and NS. NS timing system was changed to synchronize with that of Sy and gun trigger signals were modified to get time-shared for Sy and NS. The radiation safety system was also improved to fit faster alternate injection. These modifications were completed successfully in June 2013 and realized no wait injection of SR and NS. (author)

  7. Heavy ion induction linac drivers for inertial confinement fusion

    Intense beams of high energy heavy ions (e.g., 10 GeV Hg) are an attractive option for an ICF driver because of their favorable energy deposition characteristics. The accelerator systems to produce the beams at the required power level are a development from existing technologies of the induction linac, rf linac/storage ring and synchrotron. The high repetition rate of the accelerator systems, and the high efficiency which can be realized at high current make this approach especially suitable for commercial ICF. The present report gives a summary of the main features of the induction linac driver system, which is the approach now pursued in the USA. The main subsystems, consisting of injector, multiple beam accelerator at low and high energy, transport and pulse compression lines, and final focus are described. Scale relations are given for the current limits and other features of these subsystems

  8. Design considerations for high-current superconducting ion linacs

    Superconducting linacs may be a viable option for high-current applications such as fusion materials irradiation testing, spallation neutron source, transmutation of radioactive waste, tritium production, and energy production. These linacs must run reliably for many years and allow easy routine maintenance. Superconducting cavities operate efficiently with high cw gradients, properties which help to reduce operating and capital costs, respectively. However, cost-effectiveness is not the sole consideration in these applications. For example, beam impingement must be essentially eliminated to prevent unsafe radioactivation of the accelerating structures, and thus large apertures are needed through which to pass the beam. Because of their high efficiency, superconducting cavities can be designed with very large bore apertures, thereby reducing the effect of beam impingement. Key aspects of high-current cw superconducting linac designs are explored in this context

  9. Beam loading compensation for the NLC low frequency linacs

    The NLC low rf linacs are heavily loaded by a beam of about 130 ns in macropulse length (90 bunches) and a current up to 2.75 Amps. Beam loading voltage generates a large energy spread along the bunch train. This energy spread is critical for lattice design and, if not properly compensated, induces emittance growth and in turn lowers the luminosity of the machine. In this paper, the authors study the ΔF and ΔT beam loading compensation techniques for the NLC low rf linacs. They will apply these methods to the NLC low rf linacs to demonstrate the efficacy of these methods. Finally, they discuss a hybrid ΔT + ΔF method to improve the efficiency of beam loading compensation

  10. Installation of the Spallation Neutron Source (SNS) Superconducting Linac

    Stout, Daniel; Casagrande, Fabio; Cutler, Roy I; Hatfield, Daniel; Howell, Matthew; Hunter, Ted; Kersevan, Roberto; Ladd, Peter; Strong, William

    2005-01-01

    The Spallation Neutron Source (SNS) cold linac consists of 11 medium beta (0.61) and 12 high beta (0.81) superconducting RF cryomodules, 32 intersegment quadrupole magnet/diagnostics stations, 9 spool beampipes for future upgrade cryomodules, and two differential pumping stations on either side of the linac. The cryomodules and spool beampipes were designed and manufactured by Jefferson Laboratory, and the quadrupole magnets and beam position monitors were designed and furnished by Los Alamos National Laboratory. The remaining items were designed by ORNL. At present we are installing and testing the cold linac. Experience gained during installation will be presented. The performance in terms of mechanical and cryogenic systems will be described.

  11. Heavy-ion acceleration with a superconducting linac

    This year, 1988, is the tenth anniversary of the first use of RF superconductivity to accelerate heavy ions. In June 1978, the first two superconducting resonators of the Argonne Tandem-Linac Accelerator System (ATLAS) were used to boost the energy of a 19F beam from the tandem, and by September 1978 a 5-resonator linac provided an 16O beam for a nuclear-physics experiment. Since then, the superconducting linac has grown steadily in size and capability until now there are 42 accelerating structures and 4 bunchers. Throughout this period, the system was used routinely for physics research, and by now the total time with beam on target is 35,000 hours. Lessons learned from this long running experience and some key technical developments that made it possible are reviewed in this paper. 19 refs., 3 figs., 2 tabs

  12. R and D energy recovery LINAC at Brookhaven National Laboratory

    Litvinenko,V.N.; Beavis, D.; Ben-Zvi, I.; Blaskiewicz, M.; Burrill, A.; Calaga, R.; Cameron, P.; Chang, X.; Drees, A.; Ganetis, G.; Gassner, D.; Hahn, H.; Hammons, L.; Hershcovitch, A.; Hseuh, H-C.; Jain, A.; Kayran, D.; Kewisch, J.; Lambiase, R.; Lederle, D.; Mahler, G.; McIntyre, G.; Meng, W.; Nehring, T.; Oerter, B.; Pai, C.; Pate, D.; Phillips, D.; Pozdeyev, E.; Rao, T.; Reich, J.; Roser, T.; Russo, T.; Smith, K.; Tuozzolo, J.; Weiss, D.; Williams, N.; Yip, K.; Zaltsman, A.; Favale, A.; Bluem, H.; Cole, M.; Holmes, D.; Rathke, J.; Schultheiss, T.; Todd, A.; Delayen, J.; Funk, L.; Phillips, L.; Preble, J.

    2008-06-23

    Collider Accelerator Department at BNL is in the final stages of developing the 20-MeV R and D energy recovery linac with super-conducting 2.5 MeV RF gun and single-mode super-conducting 5-cell RF linac. This unique facility aims to address many outstanding questions relevant for high current (up to 0.5 A of average current), high brightness energy-recovery linacs with novel ZigZag-type merger. Recent development in the R and D ERL plans include gun and 5-cell cavity (G5) test and possibility of using R and D ERL for proof-of-principle test of Coherent Electron Cooling at RHIC.

  13. TLD determination of neutron dose contribution in medical linac

    The increased use of Linacs with accelerating voltage higher than 10 MV in clinical radiotherapy is producing and increasing demand of accurate dosimetric measurements of the photon induced neutron contamination of the radiotherapy beams, due that the associated Bremsstrahlung X rays may produce neutrons as a result of subsequent photonuclear reactions with the different materials constituting the accelerator head. Thermal neutron fluences can be measured with TLD-600/TLD-700 pairs arranged in both a bare and a cadmium (Cd) foil covered methacry-late box. Neutron response of Tl dosemeters irradiated with two different neutron sources has been investigated. The shape of the glow curve of these TLDs after irradiation in a medical Linac and in a Pu Be neutron source has been studied to verify the contribution of neutrons to an additional dose to staff, patients and the general public, due to photonuclear reactions generating neutrons from medical Linacs. (Author)

  14. A hot-spare injector for the APS linac

    Last year a second-generation SSRL-type thermionic cathode rf gun was installed in the Advanced Photon Source (APS) linac. This gun (referred to as ''gun2'') has been successfully commissioned and now serves as the main injector for the APS linac, essentially replacing the Koontz-type DC gun. To help ensure injector availability, particularly with the advent of top-up mode operation at the APS, a second thermionic-cathode rf gun will be installed in the APS linac to act as a hot-spare beam source. The hot-spare installation includes several unique design features, including a deep-orbit Panofsky-style alpha magnet. Details of the hot-spare beamline design and projected performance are presented, along with some plans for future performance upgrades

  15. Construction of an interdigital-H linac at INS

    In the radioactive-beam facility at INS, unstable nuclei with a charge-to-mass ratio greater than 1/10 are accelerated from 170 to 1046 keV/u by an interdigital-H linac. Designed IH linac consists of four acceleration tanks and three sets of quadrupole triplets placed between tanks. Output energy is continuously variable by changing rf power and phase of the last operating tank. On the basis of an equivalent circuit analysis, low power models were constructed. Resonant frequency close to the design value and flat gap voltage distribution were obtained for the tank-4 model. On the basis of the model measurement, the tank-4 for the practical use was designed and constructed. In this paper, a present status on the IH linac is described together with a brief summary of the studies done so far. (author)

  16. QCD Explorer Proposal E-Linac Versus E-Ring

    Karadeniz, H

    2006-01-01

    TeV center of mass energy lepton-hadron collider is necessary both to clarify fundamental aspects of strong interactions and for adequate interpretation of the LHC data. Recently proposed QCD Explorer utilizes the energy advantage of the LHC proton and ion beams, which allows the usage of relatively low energy electron beam. Two options for the LHC based ep collider are posibble: construction of a new electron ring in the LHC tunnel or construction of an e-linac tangentially to the LHC. In the latter case, which seems more acceptable for a number of reasons, two options are under consideration for electron linac: the CLIC technology allows shorter linac length, whereas TESLA technology gives higher luminosity.

  17. High Current Beam Dynamics in an Ess SC Linac

    Pabst, M; Letchford, A P

    2000-01-01

    Three alternative designs of the European Spallation Source (ESS) high energy linac are described. The most promising ones are either a normalconducting (nc) coupled cavity linac (CCL) up tofinal energy or a change at 407 MeV to only one group of 6 cell superconducting (sc) elliptical cavities. Fully 3d Monte Carlo simulations are presented for both options, optimized for reduced halo formation at the linac end. For the error free matched case, especially the halo formation in the longitudinal plane is more pronounced for the hybrid solution with its superconducting cavities, caused by the unavoidable phase slippage, but still quite well acceptable for loss free ring injection. Simulations however for a 30% mismatched dense core, surrounded in addition by 1.5% halo particles are showing few particles with very large amplitudes even in real space. This case represents halo formation in front to end simulations, caused by current fluctuations, filamented RFQ output distribution and enhanced by accumulated field...

  18. Penelope simulation of electron beams 6 MeV from a linear accelerator for studies in different materials equivalent to human body; Simulacion Penelope de haces de electrones de 6 MeV de un acelerador lineal para estudios en diferentes materiales equivalentes al cuerpo humano

    Apaza V, D.; Cardena R, R.; Cayllahua Q, F.; Vega R, J. [Universidad Nacional de San Agustin de Arequipa, Av. Independencia s/n, Hexagonos de Fisica, Arequipa (Peru); Urquizo B, R., E-mail: dgav02@gmail.com [Hospital Nacional Carlos Alberto Seguin Escobedo, Esquina de Peral y Filtro s/n, Arequipa (Peru)

    2015-10-15

    In systems of radiotherapy treatment for cancer, always looking to maximize the radiation dose on the target (tumor) and minimize to the organs at risk or healthy, so they resort to using electron beams that have properties and characteristics of higher dose deposition at fixed depths, directing and focusing the higher dose in the tumor, without harming healthy tissues to which seeks to radiate in the least possible. Simulating the interaction of electron beams with different equivalent tissues to the human body leads to a better dosimetric evaluation, improving the quality of treatment planning. The aim of this study is the comparison from the characterization of several equivalent tissues to the human body such as soft tissue, bone and lung. Based on the simulation of a calibration beam in water phantom with Penelope code and compared with the results of the calibration curves of beams in water vat by a linear accelerator Elekta Synergy of Hospital Nacional Carlos Alberto Seguin Escobedo EsSalud of Arequipa (Peru). From this to evaluate the behavior of electron beams in a homogeneous medium and then further evaluation in the human body homogeneities, for better evaluation and specific treatment planning. (Author)

  19. Simulation of dose deposition in heterogeneities in the human body, using the Penelope code for photons beams of energies of a linear accelerator; Simulacion de la deposicion de dosis en las heterogeneidades del cuerpo humano, usando el codigo Penelope para haces de fotones de energias de un acelerador lineal

    Cardena R, A. R.; Vega R, J. L.; Apaza V, D. G., E-mail: cardroj@yahoo.es [Universidad Nacional de San Agustin, Av. Independencia s/n, Arequipa (Peru)

    2015-10-15

    The progress in cancer treatment systems in heterogeneities of human body has had obstacles by the lack of a suitable experimental model test. The only option is to develop simulated theoretical models that have the same properties in interfaces similar to human tissues, to know the radiation behavior in the interaction with these materials. In this paper we used the Monte Carlo method by Penelope code based solely on studies for the cancer treatment as well as for the calibration of beams and their various interactions in mannequins. This paper also aims the construction, simulation and characterization of an equivalent object to the tissues of the human body with various heterogeneities, we will later use to control and plan experientially doses supplied in treating tumors in radiotherapy. To fulfill the objective we study the ionizing radiation and the various processes occurring in the interaction with matter; understanding that to calculate the dose deposited in tissues interfaces (percentage depth dose) must be taken into consideration aspects such as the deposited energy, irradiation fields, density, thickness, tissue sensitivity and other items. (Author)

  20. Calculation of the structural shielding of the radiotherapy treatment room equipped with a linear accelerator type Tomo therapy Hi-Art in the Oncology Center of Chihuahua, Mexico; Calculo del blindaje estructural de la sala de tratamiento de radioterapia equipada con un acelerador lineal del tipo Tomotherapy Hi-Art en el Centro Oncologico de Chihuahua, Mexico

    Caballero G, C. A. [Southwest Oncology Centers, North Civic Center Plaza No. 2926, Scottsdale, Arizona (United States); Plascencia, J. C. [Centro Oncologico Louis and Lucille Grado, Republica del Peru No. 102-5, Col. Americas, Aguascalientes (Mexico); Vargas V, M. X.; Toledo J, P., E-mail: cabshm@msn.co [Centro Oncologico de Chihuahua, Hacienda de la Esperanza No. 6304, Fracc. Cima Comercial, Chihuahua (Mexico)

    2010-09-15

    The helicoid tomo therapy is an external radiotherapy system of modulated intensity, guided by image, in which the radiation is imparted to the patient using a narrow radiation beam in helicoid form, in a similar way to the scanning process with a computerized tomography. The tomo therapy equipment (Tomo Therapy Hi-Art) consists in an electrons linear accelerator with acceleration voltages of 6 MV for treatment and 3.5 MV for image, coupled to a ring that turn around the patient as this is transferred through this ring in perpendicular sense to the radiation beam. The radiation beam is narrow because has the maximum size of 5 x 40 cm{sup 2} in the isocenter. The intensity modulation of the beam is carried out with a binary dynamic collimator of 64 crisscross sheets, and the guide by image though a system of megavoltage computerized tomography. Opposed to the radiation beam, also coupled to the rotational ring, a group of lead plates exists with a total thickness of 13 cm that acts as barrier of the primary radiation beam. The special configuration of the tomography equipment makes to have the following characteristics: 1) the presence of the lead barrier of the equipment reduces the intensity of the primary beam that reaches the bunker walls in considerable way, 2) the disperse and leakage radiations are increased with regard to a conventional accelerator due to the increase in the necessary irradiation time to produce modulated intensity fields by means of the narrow radiation beam. These special characteristics of the tomo therapy equipment make that particularities exist in the application of the formulations for structural shielding calculations that appears in the NCRP reports 49, NCRP 151 and IAEA-SRS-47. For this reason, several researches have development analytic models based on geometric considerations of continuous rotation of the equipment ring to determine the shielding requirements for the primary beam, the dispersed and leakage radiation in tomo therapy. In this work these specific methodologies are used for the structural shielding calculations of the tomo therapy equipment installed in the Oncology Center of Chihuahua. These calculation methodologies consider the primary radiation, of leakage, disperse, second dispersion and leakage dispersion. The obtained results indicate that due to the lead barrier of the primary beam, the main component that contributes to the shielding requirements of the installation is the leakage radiation. On the other hand, the component that more affects of the door shielding is the dispersion component in the patient. (Author)

  1. Predicción no lineal de caudales medios mensuales usando funciones de influencia radial y técnicas espectrales.

    Rojo Hernández, Julián David; Carvajal Serna, Luis Fernando

    2012-01-01

    La estrecha relación no lineal entre los caudales y los procesos climáticos de escala global justifican la modelación no lineal para la predicción de caudales. El presente trabajo muestra una aproximación a la dinámica no lineal de los caudales usando un modelo no paramétrico de regresión basado en las funciones de influencia radial y técnicas de descomposición espectral. El modelo propuesto es aplicado para la predicción de los caudales medios mensuales para horizontes de pronóstico de 1,3 y...

  2. Approach of a failure analysis for the MYRRHA linac

    The MYRRHA project currently under development at SCK-CEN (Mol, Belgium) is a subcritical research reactor that requires a 600 MeV proton accelerator as a driver. This linac is expected to produce a beam power of 1.5 MW onto a spallation target for the reactor to deliver a thermal power around 70 MW. Thermomechanical considerations of the spallation target set stringent requirements on the beam trip rate which should not exceed 40 trips/year for interruptions longer than three seconds. The 3 underlying principles in the design of the MYRRHA linac are elements redundancy (like the dual-injector), elements operation at de-rated values (like cavities operating at about 30% from their nominal operating points) and the fault tolerance concept, which allows the failure of a beamline component to be compensated by its neighbouring elements. Studies presented in this document show that in the event of a failure of the first cryo-module or the first quadrupole doublet the linac can resume nominal operation with a re-matched lattice. Since the fault tolerance procedure is expected to work more efficiently at higher energies (due to lower space charge effects) we can extrapolate from our studies that the MYRRHA linac is expected to operate with the failure of any cryo-module or quadrupole doublet in the main linac. A virtual accelerator-based control system is mandatory for the operation of the MYRRHA linac to ensure the very fast implementation (<3 seconds) of the fault tolerance procedure. The virtual accelerator uses a beam dynamics code (like TRACEWIN or TRACK) to compute the model of the real accelerator in operation and interacts with this later through the accelerator control command

  3. An energy recovery electron linac-on-ring collider

    Merminga, L.; Krafft, G.A.; Lebedev, V.A.; Ben-Zvi, I.

    2000-09-14

    We present the design of high-luminosity electron-proton/ion colliders in which the electrons are produced by an Energy Recovering Linac (ERL). Electron-proton/ion colliders with center of mass energies between 14 GeV and 100 GeV (protons) or 63 GeV/A (ions) and luminosities at the 10{sup 33}(per nucleon) level have been proposed recently as a means for studying hadronic structure. The linac-on-ring option presents significant advantages with respect to: (1) spin manipulations (2) reduction of the synchrotron radiation load in the detectors (3) a wide range of continuous energy variability. Rf power and beam dump considerations require that the electron linac recover the beam energy. Based on extrapolations from actual measurements and calculations, energy recovery is expected to be feasible at currents of a few hundred mA and multi-GeV energies. Luminosity projections for the linac-ring scenario based on fundamental limitations are presented. The feasibility of an energy recovery electron linac-on-proton ring collider is investigated and four conceptual point designs are shown corresponding to electron to proton energies of: 3 GeV on 15 GeV, 5 GeV on 50 GeV and 10 GeV on 250 GeV, and for gold ions with 100 GeV/A. The last two designs assume that the protons or ions are stored in the existing RHIC accelerator. Accelerator physics issues relevant to proton rings and energy recovery linacs are discussed and a list of required R and D for the realization of such a design is presented.

  4. Improved cathode assembly for electron gun of 7 MeV linac

    This Electron Beam Linear Accelerator (LINAC) of RPCD, BARC is the key component of the pulse radiolysis facility being used for radiation chemistry research. The heart of the LINAC is the electron gun, which generates electron from a tungsten cathode. Recently an improved cathode assembly is designed and fabricated for better performance of the linac. (author)

  5. Thermal simulation of linac cavity of 10 MeV RF linac

    The 10 MeV RF linac at Electron Beam Centre Kharghar, has 33 cells assembly fabricated in three parts. Of these, the top and the bottom parts consist of 14 cells each while the middle part has 5 cells, including the power feed cavity. Water cooling is provided to the cavity by brazing Cu tube spirally over the cavity surface. Detailed conjugate heat transfer modelling has been carried out using the FLUENT flow modelling software. The temperature distribution profile is obtained which identify the hot spot zones. The further thermal optimization has been carried out based on the results and more uniform thermal profile is obtained by modification in the cooling tubes design and water flow rate. (author)

  6. Neutron distribution and induced activity inside a Linac treatment room.

    Juste, B; Miró, R; Verdú, G; Díez, S; Campayo, J M

    2015-08-01

    Induced radioactivity and photoneutron contamination inside a radiation therapy bunker of a medical linear accelerator (Linac) is investigated in this work. The Linac studied is an Elekta Precise electron accelerator which maximum treatment photon energy is 15 MeV. This energy exceeds the photonuclear reaction threshold (around 7 MeV for high atomic number metals). The Monte Carlo code MCNP6 has been used for quantifying the neutron contamination inside the treatment room for different gantry rotation configuration. Walls activation processes have also been simulated. The approach described in this paper is useful to prevent the overexposure of patients and medical staff. PMID:26737878

  7. Billion particle linac simulations for future light sources

    In this paper we report on multi-physics, multi-billion macroparticle simulation of beam transport in a free electron laser (FEL) linac for future light source applications. The simulation includes a self-consistent calculation of 3D space-charge effects, short-range geometry wakefields, longitudinal coherent synchrotron radiation (CSR) wakefields, and detailed modeling of RF acceleration and focusing. We discuss the need for and the challenges associated with such large-scale simulation. Applications to the study of the microbunching instability in an FEL linac are also presented

  8. SRF cavities for CW option of Project X Linac

    Solyak, N.; Gonin, I.; Khabiboulline, T.; Lunin, A.; Perunov, N.; Yakovlev, V.; /Fermilab

    2009-09-01

    Alternative option of Project X is based on the CW SC 2GeV Linac with the average current 1mA. Possible option of the CW Linac considered in the paper includes low energy part consisted of a few families SC Spoke cavities (from 2.5 MeV to 466 MeV) and high energy part consisted of 2 types of elliptical cavities (v/c=0.81 and v/c=1). Requirements and designed parameters of cavities are considered.

  9. Tranverse beam break up in a periodic linac

    The problem of cumulative beam break up in a periodic linac for a general impedance is discussed, with the effects of acceleration included. The transverse equations of motion for a set of identical point like bunches moving along the length of the linac are cast into a simple form using a smooth approximation. This results in a working formula that is used to analyze beam breakup. Explicit expressions for the transverse motion in the case of a single resonance impedance are found using saddle point integration. This is done first with no external focusing, and again in the strong focusing limit

  10. Beam Instrumentation Using BPM System of the SPring-8 Linac

    Yanagida, K; Dewa, H; Hanaki, H; Kobayashi, T; Mizuno, A; Suzuki, S; Taniuchi, T; Tomizawa, H

    2004-01-01

    A beam position monitor (BPM) system of the SPring-8 linac has been operated since 2002. The following upgrade programs have been carried out during this period: The BPMs were installed in the linac's dispersive sections. A synchronized accumulation of beam position data into the database system started. A feedback control of steering magnets for beam position stabilization has been under development. In this conference the authors report a performance of the BPM system, and discuss its usefulness for beam diagnostics, machine diagnostics and beam stabilization.

  11. Optical laser systems at the Linac Coherent Light Source

    Minitti, Michael P.; Robinson, Joseph S.; Coffee, Ryan N.; Edstrom, Steve; Gilevich, Sasha; Glownia, James M.; Granados, Eduardo; Hering, Philippe; Hoffmann, Matthias C.; Miahnahri, Alan; Milathianaki, Despina; Polzin, Wayne; Ratner, Daniel; Tavella, Franz; Vetter, Sharon; Welch, Marc; White, William E.; Fry, Alan R., E-mail: alanfry@slac.stanford.edu [Linac Coherent Light Source, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025 (United States)

    2015-04-22

    This manuscript serves as a reference to describe the optical laser sources and capabilities at the Linac Coherent Light Source. Ultrafast optical lasers play an essential role in exploiting the unique capabilities of recently commissioned X-ray free-electron laser facilities such as the Linac Coherent Light Source (LCLS). Pump–probe experimental techniques reveal ultrafast dynamics in atomic and molecular processes and reveal new insights in chemistry, biology, material science and high-energy-density physics. This manuscript describes the laser systems and experimental methods that enable cutting-edge optical laser/X-ray pump–probe experiments to be performed at LCLS.

  12. Linac Beam Dynamics Simulations With PY-ORBIT

    Linac dynamics simulation capabilities of the PyORBIT code are discussed. PyORBIT is an open source code and a further development of the original ORBIT code that was created and used for design, studies, and commissioning of the SNS ring. The PyORBIT code, like the original one, has a two-layer structure. C++ is used to perform time-consuming computations, and the program flow is controlled from a Python language shell. The flexible structure makes it possible to use PyORBIT also for linac dynamics simulations. A benchmark of PyORBIT with Parmila and the XAL Online model is presented.

  13. Coupled cavity 3-D codes for linac tolerance simulations

    Three developing codes, based on previous work at Los Alamos (1) are now being used in the Fermilab Linac Upgrade project, to survey system tolerance requirements. Both linear and non-linear beam dynamics of a pi-mode side coupled 805 MHz linac are simulated. Particular attention to the z-plane synchronism has been integrated into the code group, so that klystron drive boundaries can be monitored in the dynamics. All system length errors that contribute to desynchronization, and other data set failures are recognized by the particle PIC code (CAVDYN) to enhance design coherence. Some current results of the CAVDYN code simulations will be discussed

  14. Estimates of dispersive effects in a bent NLC Main Linac

    Michael Syphers and Leo Michelotti

    2000-10-31

    An alternative being considered for the Next Linear Collider (NLC) is not to tunnel in a straight line but to bend the Main Linac into an arc so as to follow a gravitational equipotential. The authors begin here an examination of the effects that this would have on vertical dispersion, with its attendant consequences on synchrotron radiation and emittance growth by looking at two scenarios: a gentle continuous bending of the beam to follow an equipotential surface, and an introduction of sharp bends at a few sites in the linac so as to reduce the maximum sagitta produced.

  15. Beam Loading Compensation in the Main Linac of CLIC

    Schulte, D.; Syratchev, I.

    2000-01-01

    Compensation of multi-bunch beam loading is of great importance in the main linac of the Compact Linear Collider (CLIC). The bunch-to-bunch energy variation has to stay below 1 part in 1000. In CLIC, the RF power is obtained by decelerating a drive beam which is formed by merging a number of short bunch trains. A promising scheme for tackling beam loading in the main linac is based on varying the lengths of the bunch trains in the drive beam. The scheme and its expected performance are presen...

  16. Sobre el uso del problema de complementariedad lineal extendido para el control óptimo de semáforos

    Lema Fernández, Carmen S.

    2007-01-01

    Full Text Available En el trabajo titulado “Modelo de optimización con restricciones de equilibrio para el control de semáforos” que presentamos en las XIV Jornadas de ASEPUMA (2006 analizábamos un problema de control óptimo de semáforos para un cruce de dos carreteras con los dos sentidos de circulación; allí interpretábamos las restricciones del problema como un problema de complementariedad lineal extendido (ELCP. También proponíamos un método híbrido de solución basado en una propiedad que demostraba que mediante un cambio de variable adecuado, las restricciones de ELCP describen un problema de complementariedad lineal (LCP. Nos interesa pues, estudiar bajo que condiciones dichos problemas tienen solución y además única. Así introducimos tres propiedades importantes para los ELCP y como caso particular para los LCP:• La propiedad de suficiencia en columnas que caracteriza la convexidad del conjunto solución.• La propiedad de suficiencia en filas que describe una clase importante de pares de matrices (respecto a K para las cuales la factibilidad del ELCP(M,N,K implica su solucionabilidad.• La P-propiedad (que para el caso del LCP(M,q significa que M ha de ser una P-matriz, que caracteriza la unicidad de solución.

  17. Design and construction of the main linac module for the superconducting energy recovery linac project at Cornell

    Cornell University has been designing and building superconducting accelerators for various applications for more than 50 years. Currently, an energy-recovery linac (ERL) based synchrotron-light facility is proposed making use of the existing CESR facility. As part of the phase 1 R and D program funded by the NSF, critical challenges in the design were addressed, one of them being a full linac cryo-module. It houses 6 superconducting cavities- operated at 1.8 K in continuous wave (CW) mode - with individual HOM absorbers and one magnet/ BPM section. Pushing the limits, a high quality factor of the cavities (2⋅1010) and high beam currents (100 mA accelerated plus 100 mA decelerated) are targeted. We will present the design of the main linac cryo-module (MLC) being finalized recently, its cryogenic features and report on the status of the fabrication which started in late 2012

  18. Comprensión del concepto combinación lineal de vectores desde el punto de vista de la teoría APOE

    Parraguez, Marcela

    2011-01-01

    La investigación se sitúa en el estudio del concepto combinación lineal de vectores, que concierne al álgebra lineal, bajo un enfoque cognitivo donde se utiliza la teoría APOE como marco teórico y metodológico. Las tres componentes propuestas por este ciclo de investigación determinan la estructura general del estudio. En la parte empírica de esta investigación se diseñó y aplicó un cuestionario y entrevistas a 8 estudiantes del programa de Licenciatura en Matemáticas de la Pontificia Univers...

  19. Introducción suave a ideas fundamentales para resolver problemas de programación lineal en enteros por medio de matemáticas recreativas

    M. A. Murray Lasso

    2005-01-01

    Los algoritmos de corte de Gomory para resolver programas lineales en enteros tienen que encontrar una solución entera a un programa lineal obtenido del orig inal al que se le hicieron unos “cortes.” La presentacion en los textos de dichos algoritmos, generalmente son muy abstractas y difíciles de seguir, máxime que pocos textos presentan ejemplos en todo detalle donde se vea exactamente qué hace cada corte. En este artículo, se muestran varios ejemplos con soluciones detalladas y con una com...

  20. Metodología para el estudio geotécnico en fase de proyecto de grandes desmontes en roca alterada de obras lineales.

    Farfán Martín, Arturo

    2011-01-01

    [ES] La contratación del estudio geotécnico en fase de proyecto de grandes desmontes en roca de obras lineales, en España, se legisla por los Pliegos de prescripciones técnicas particulares realizados por la entidad que saca a concurso la licitación de toda la obra lineal, en los que se cita la forma de abordar el estudio geotécnico del corredor, tanto de los desmontes como de los terraplenes, desde un punto de vista genérico. Esto genera una serie de problemas de indefinición a la hora de...

  1. Dificultades que presentan los estudiantes en los modos geométrico y analítico de sistemas de ecuaciones lineales

    García, Carlos; Oktaç, Asuman; Ramírez, Carina

    2006-01-01

    En este trabajo presentamos algunas dificultades que tienen los estudiantes en la representación gráfica de sistemas de ecuaciones lineales con dos variables. Para ello, se diseñó una entrevista basándonos en el acercamiento teórico de los modos de pensamiento geométrico y analítico en álgebra lineal. Reportamos acerca del desempeño de los estudiantes ante situaciones presentadas en un modo geométrico.

  2. Aproximación no lineal al modelo de overshooting usando redes neuronales multicapa para el tipo de cambio dólar - peso

    Jaime Villamil

    2009-01-01

    Desde los años setenta muchos trabajos han intentado elaborar una sustentación empírica de algunos modelos
    que ofrecieron una explicación lineal de la dinámica de la tasa de cambio de un país, entre ellos el de Dornbusch. Hasta el momento ninguno ha sido concluyente y la caminata aleatoria es considerada como el mejor modelo al que puede ajustarse. De Grauwe ha mostrado que, con la presencia de relaciones no-lineales y heterogeneidad de expectativas de los especuladores, el tipo de...

  3. Propuesta didáctica para la enseñanza de los métodos para resolver un sistema de ecuaciones lineales

    Rojas, Jorge; Ariza, Alejandra

    2013-01-01

    Este artículo pretende evidenciar la importancia que tiene la enseñanza de los métodos para resolver sistemas de ecuaciones lineales, de manera posterior a la función lineal, para esto se trabajará como metodología la teoría de situaciones didácticas de Brousseau, buscando la construcción propia de cada estudiantes, generando en ellos un aprendizaje significativo; esto se buscará a partir de un contexto familiar para ellos, impulsando las buenas aptitudes de los estudiantes y el ánimo para en...

  4. Análisis de la dinámica no lineal y cambios de complejidad en la variabilidad del ritmo cardiaco

    Valencia Murillo, José Fernando; Vallverdú Ferrer, Montserrat; Caminal Magrans, Pere

    2010-01-01

    Se han desarrollado y aplicado unas nuevas metodologías para estimar la complejidad de la variavilidad del ritmo cardiaco, las cuales facilitan la obtención de un mejor diagnóstico de las enfermedades cardiacas y ayudan en la detección de riesgo de sufrir muerte cardiaca. Considerendo la evidencia de determinismo no lineal y no predictivo de las series RR, las metodologías desarrolladas están basadas en técnicas de la dinamica no lineal para la obtención de índices que permitan medir la influ...

  5. Equacions efectives de l'equació de Schrödinger no lineal en sistemes periòdics i quasiperiòdics

    Monreal Mengual, Llucía

    2010-01-01

    El propósito de esta tesis se enmarca dentro del campo de la óptica no lineal y, como el problema es formalmente idéntico, tiene aplicación directa en el campo de la materia condensada, en particular en los condensados de Bose-Einstein. El objetivo es obtener una nueva herramienta teórica que permita analizar la dinámica de una solución no lineal estacionaria sometida a una perturbación pequeña. Nos centraremos en soluciones que llenen todos los nodos de la red, y, por lo tanto, que tienen si...

  6. APF-IH type linac for PIXE analysis

    We are studying an APF-IH type linac for PIXE analysis use. The compact (L=1.5m) linac accelerate proton from 40 keV to 2.0 MeV. This APF (Alternating-Phase-Focus) system can not focus so high intense beam, but beam of several 100 μA is focused by combination of Focus-Defocus sequence. For PIXE analysis, intensity of bombard particles are several μA lower than several 100 μA. From particle orbit calculation, on energy width of ±0.25%, this linac can accept transverse emittance of 113 πmm·mrad, longitudinal phase of 35deg (by using a buncher, beam transmission get larger than 65%) and beam intensity of several 100 μA. The linac can accelerate proton to 2.0 MeV by RF power of about 10 kW. We designed the Interdigital H (IH) leaner accelerator by particle-orbit calculation. All PIXE analysis system occupy only 2mx3m. A half-model cavity was designed. The model is manufacturing now for measurement of RF characteristics. (author)

  7. Supervisory control system for 10 MeV linac

    A 10 MeV Linac is being tested at Raja Ramanna Centre for Advanced Technology. The Linac system consists of subsystems like RF system, magnet power supplies, vacuum pumps and gauges, radiation monitoring systems, interlocks and personnel safety system and the support systems required for the operation of Linac. A supervisory control system for Linac and associated subsystems is developed at Raja Ramanna Centre for Advanced Technology. The control system features monitoring and controls of diversified subsystems, timing trigger system, synthesizer, oscilloscopes, machine and personnel safety interlocks. The control system hardware is VME bus based controller referred to as the Equipment controller (EC). All the subsystems are interfaced to the EC with isolation in each interface signal. Interlocks are supervised directly in hardware. Personnel safety is ensured by the 'Area Search' interlock. The software layer of the control system consists of a server and client based Supervisory Control And Data Acquisition (SCADA) system implemented in LabView. Software system also includes GUI at operator console and dedicated softwares developed to control various instruments connected on Ethernet. The server interacts with the EC over RS232 link. A Web site is also developed to locally display the historical data of beam current, beam energy and facilitates the retrieval of the various parameter values logged in the data base. The paper describes the architecture of control system, the hardware and software developments, features and operational experiences. (author)

  8. MAFIA analysis of the effects of coupling slots in linacs

    Adams, F. P.; Ungrin, J.; de Jong, M. S.

    1991-05-01

    We have used the MAFIA codes to analyze on-axis slot-coupled {π}/{2}- mode standing-wave linac structures. Quadrupolar fields in the structure are found to produce an elliptical accelerated beam. A modification to the design, yielding reduced beam ellipticity, is proposed.

  9. Full power to the first Linac4 module

    Francesco Poppi

    2010-01-01

    Since last week the first of a total of 23 accelerating structures for Linac4 has been undergoing high-power tests. Although still a prototype, this structure is destined to be the first of the 12 PIMS cavities to be installed in the Linac4 tunnel and it has been completely designed, developed and constructed at CERN.   The PIMS prototype. The new Linac4 has 4 different types of accelerating structures. The PI-Mode Structures (PIMS) are the last stage and are designed to accelerate protons up to 160 MeV. “PIMS have never before been used to accelerate protons”, explains Frank Gerigk, the project engineer responsible for the Linac4 accelerating structures. “In LEP, they were used to accelerate electrons, and now we have modified them and improved several design features to make them suitable for protons”. The first prototype was entirely manufactured in the CERN workshop. Due to the size of the pieces it was difficult to achieve and preserve the required to...

  10. SRF LINAC for future extension of the PEFP

    A study on the superconducting RF linac is underway in order to increase the beam energy up to 1 GeV by extending the Proton Engineering Frontier Project (PEFP) 100-MeV linac. The operating frequency of the PEFP superconducting linac (SCL) is 700 MHz, which is determined by the fact that the frequency of the existing normal conducting linac is 350 MHz. A preliminary study on the beam dynamics showed that two types of cavities with geometrical betas of 0.50 and 0.74 could cover the entire energy range from 100 MeV to 1 GeV. An inductive output tube (IOT) based RF system is under consideration as a high-power RF source for the SCL due to its low operating voltage and high efficiency. As a prototyping activity for a reduced beta cavity, a five-cell cavity with a geometrical beta of 0.42 was designed and fabricated. A vertical test of the prototype cavity at low temperatures was performed to check the performance of the cavity. The design study and the prototyping activity for the PEFP SCL will be presented in this paper.

  11. 200 MeV RF linac for synchrotron injection

    Construction has been completed on an electron linear accelerator for the Brookhaven National Laboratory. This accelerator will be used for the injection of a 200 MeV electron beam into a synchrotron for lithography experiments. This paper describes the conceptual design of the linac, its e-gun pulser, and its control and timing systems. 3 figs., ref

  12. Beam dynamics of alternating-phase-focused linac

    Iwata, Y; Kapin, V

    2004-01-01

    A simple method to find an array of synchronous phases for alternating-phase-focused (APF) linacs is presented. The phase array is described with a smooth function having free parameters. With a set of the parameters, a simulation on the beam dynamics was made and distributions of the six-dimensional phase spaces were calculated for each set of the parameters. The parameters were varied, and numbers of the simulations have been performed. An optimum set of the parameters were determined so that the simulations of the beam dynamics yield large acceptances and small emittances of the extracted beams. Since the APF linac can provide both axial and radial stability of beams just with the rf acceleration-field, no additional focusing element inside of drift tubes are necessary. Comparing with conventional linacs having focusing elements, it has advantage in construction and operation costs as well as its acceleration rate. Therefore, the APF linacs would be suited for an injector of medical synchrotrons. A practic...

  13. Design study on an intense heavy-ion linac system

    A four-vane RFQ cavity is designed for an intense heavy-ion linac system. RFQ-vanes with small tip curvatures are applied in order to improve the RF power efficiency. Beam optical and RF parameters are investigated by beams of numerical methods. Using a scale model, the cavity structure is experimentally optimized. (Author) 7 refs., 4 figs

  14. SRF LINAC for future extension of the PEFP

    Kim, Han Sung; Kwon, Hyeok Jung; Seol, Kyoung Tae; Jang, Ji Ho; Cho, Yong Sub [Proton Engineering Frontier Project, Korea Atomic Energy Research Institute, Daejeon (Korea, Republic of)

    2014-04-15

    A study on the superconducting RF linac is underway in order to increase the beam energy up to 1 GeV by extending the Proton Engineering Frontier Project (PEFP) 100-MeV linac. The operating frequency of the PEFP superconducting linac (SCL) is 700 MHz, which is determined by the fact that the frequency of the existing normal conducting linac is 350 MHz. A preliminary study on the beam dynamics showed that two types of cavities with geometrical betas of 0.50 and 0.74 could cover the entire energy range from 100 MeV to 1 GeV. An inductive output tube (IOT) based RF system is under consideration as a high-power RF source for the SCL due to its low operating voltage and high efficiency. As a prototyping activity for a reduced beta cavity, a five-cell cavity with a geometrical beta of 0.42 was designed and fabricated. A vertical test of the prototype cavity at low temperatures was performed to check the performance of the cavity. The design study and the prototyping activity for the PEFP SCL will be presented in this paper.

  15. Heavy ion linac as a high current proton beam injector

    Barth, Winfried; Adonin, Aleksey; Appel, Sabrina; Gerhard, Peter; Heilmann, Manuel; Heymach, Frank; Hollinger, Ralph; Vinzenz, Wolfgang; Vormann, Hartmut; Yaramyshev, Stepan

    2015-05-01

    A significant part of the experimental program at Facility for Antiproton and Ion Research (FAIR) is dedicated to pbar physics requiring a high number of cooled pbars per hour. The primary proton beam has to be provided by a 70 MeV proton linac followed by two synchrotrons. The new FAIR proton linac will deliver a pulsed proton beam of up to 35 mA of 36 μ s duration at a repetition rate of 4 Hz (maximum). The GSI heavy ion linac (UNILAC) is able to deliver world record uranium beam intensities for injection into the synchrotrons, but it is not suitable for FAIR relevant proton beam operation. In an advanced machine investigation program it could be shown that the UNILAC is able to provide for sufficient high intensities of CH3 beam, cracked (and stripped) in a supersonic nitrogen gas jet into protons and carbon ions. This advanced operational approach will result in up to 3 mA of proton intensity at a maximum beam energy of 20 MeV, 1 0 0 μ s pulse duration and a repetition rate of up to 2.7 Hz delivered to the synchrotron SIS18. Recent linac beam measurements will be presented, showing that the UNILAC is able to serve as a proton FAIR injector for the first time, while the performance is limited to 25% of the FAIR requirements.

  16. New control system for the KEK-linac

    New control system for the KEK-Linac has been developed. Unix-based workstations and VME-bus computers are introduced. They are inter-connected with an Ethernet, which is used as a high-speed data-exchange network. New system will start the operation after October 1993. (author)

  17. Optimization of steering elements in the RIA driver linac

    The driver linac of the projected RIA facility is a versatile accelerator, a 1.4-GV, CW superconducting (SC) linac designed to simultaneously accelerate several heavy-ion charge states, providing beams from proton to uranium at 400 MeV/u at power levels at a minimum of 100 kW and up to 400 kW for most beams. Acceleration of multiple-charge-state uranium beams places stringent requirements on the linac design. A steering algorithm was derived that fulfilled the driver's real estate requirements, such as placement of steering dipole coils on SC solenoids and of beam position monitors outside cryostats, and beam-dynamics requirements, such as coupling effects induced by the focusing solenoids. The algorithm has been fully integrated into the tracking code TRACK and it is used to study and optimize the number and position of steering elements that minimize the multiple-beam centroid oscillations and preserve the beam emittance under misalignments of accelerating and transverse focusing elements in the driver linac

  18. Linac4: injecting new life into the LHC

    Antonella Del Rosso

    2015-01-01

    Construction work is nearing completion on the ion source for Linac4, the new linear accelerator that forms part of the LHC injector upgrade programme. Here we find out more about this essential component of the accelerator chain, designed and built at CERN.     The image shows the Linac4 H- source. The red light is the alpha line of the visible hydrogen emission spectrum. The ion source is a key component of Linac4, the linear accelerator that from 2018 will supply H- ions (hydrogen atoms with an extra electron) at 160 MeV for injection into the accelerator complex. As the only ion source at CERN, Linac4 must be highly reliable, which requires a full understanding of the production mechanisms, the simulation of physical processes and the validation of those processes through experimentation. “This source is the result of much fruitful collaboration,” says Jacques Lettry of the BE department. “Its design was inspired by the many sources of th...

  19. RADIATION PROTECTION OF LINAC BUNKERS. A USER-FRIENDLY APPROACH

    Holten Sørensen, Thyge; Olsen, Kjeld Jørgen; Behrens, Claus Flensted

    2015-01-01

    A well-known but complex formalism for the calculation of the leakage dose at the entrance of the linac maze was considered and simplified. These simplifications were based partly on the literature and partly on the authors' own measurements. The authors have included photon scatter originating f...

  20. Design and analysis of X-band femtosecond linac

    Uesaka, M.; Kozawa, T.; Takeshita, A.; Kobayashi, T.; Ueda, T.; Miya, K. [Tokyo Univ., Tokai, Ibaraki (Japan). Nuclear Engineering Research Lab.

    1997-03-01

    Femtosecond quantum phenomena research project is proposed at Nuclear Engineering Research Laboratory, University of Tokyo. The research facility consists of an X-band (11.424GHz) femtosecond electron linac, a femtosecond wavelength tunable laser, two S-band (2.856GHz) picosecond electron linacs and measuring equipments. Especially, we aim to generate a 100 fs (FWHM) electron single bunch with more than 1 nC at the X-band femtosecond linac. Ultrafast processes in radiation physics, chemistry, material science and microscopic electromagnetic phenomena are going to be analyzed there. Here the design and analysis of an X-band femtosecond linac is presented. The simulation of electron dynamics is carried out including magnetic pulse compression by using PARMELA and SUPERFISH. It is found by the simulation that the 600 ps (tail-to-tail) electron emission from a 200 kV thermionic gun can be bunched and compressed to 110 fs (FWHM) with the charge of 0.8 nC which gives 7.3 kA. We plan to use one high power X-band klystron which can supply 60 MW with more than 200 ns pulse duration. The flatness of plateau of the pulse should be 0.2% for stable ultrashort bunch generation. (author)

  1. Failure Modes Analysis for the MSU-RIA Driver Linac

    Wu, Xiaoyu; Gorelov, Dmitry; Grimm, Terry L; Marti, Felix; York, Richard

    2005-01-01

    Previous end-to-end beam dynamics simulation studies* using experimentally-based input beams including alignment and rf errors and variation in charge-stripping foil thickness have indicated that the Rare Isotope Accelerator (RIA) driver linac proposed by MSU has adequate transverse and longitudinal acceptances to accelerate light and heavy ions to final energies of at least 400 MeV/u with beam powers of 100 to 400 kW. During linac operation, equipment loss due to, for example, cavity contamination, availability of cryogens, or failure of rf or power supply systems, will lead to at least a temporary loss of some of the cavities and focusing elements. To achieve high facility availability, each segment of the linac should be capable of adequate performance even with failed elements. Beam dynamics studies were performed to evaluate the linac performance under various scenarios of failed cavities and focusing elements with proper correction schemes, in order to prove the flexibility and robustness of the driver ...

  2. Status update on the photocathode RF LINAC project

    We present the progress achieved so far in the Photocathode Linac Project. We have developed and tested linear accelerator structures at 2856 MHz, designed and performed preliminary tests on the photocathode gun, commissioned the klystron modulator and microwave systems to extract 3.2 MW of pulsed power, developed the beam-line, and are ready to commence acceleration experiments. (author)

  3. A low-charge-state injector linac for ATLAS

    The design of a low-charge-state linac which is capable of accelerating, for example, 132Sn1+ for injection into the existing heavy-ion linac ATLAS is discussed. The injector linac is intended for radioactive beam applications, and will accelerate a low- charge-state beam to energies of 500 keV/nucleon, at which point the ions can be stripped to charge states sufficiently high to be injected into ATLAS. A primary design goal has been to extend the very good longitudinal beam quality typical of ATLAS to low charge state beams. The proposed injector linac consists of several elements. First is a gridded-gap four-harmonic buncher and a short (normally-conducting) 12 MHz RFQ structure, both operating on a 350 kV open-air variable-voltage platform. Then comes an array of 24 Mhz and 48 Mhz superconducting interdigital accelerating structures interspersed with superconducting quadrupole transverse focusing elements. Numerical ray-tracing studies indicate that a transverse acceptance greater than 0.25π mm-mrad can be obtained while simultaneously limiting longitudinal emittance growth to a very few keV-nsec

  4. Status of the Project-X CW Linac Design

    Ostiguy, J-F.; Solyak, N.; Berrutti, P.; Carneiro, J.P.; Lebedev, V.; Nagaitsev, S.; Saini, A.; Stheynas, B.; Yakovlev, V.P.; /Fermilab

    2012-05-01

    Project-X is a proposed proton accelerator complex at Fermilab that would provide particle beams to support a diversified experimental program at the intensity frontier. As currently envisioned, the complex would employ a CW superconducting linac to accelerate a 1 mA average, 5 mA peak H{sup -} beam from 2.1 MeV to 3 GeV. A second superconducting linac, operating in pulsed mode would ultimately accelerate a small fraction of this beam up to 8 GeV. The CW linac is based on five families of resonators operating at three frequencies: half-wave (1 family at 162.5 MHz), spoke (2 families at 325 MHz) and elliptical (2 families at 650 MHz). Accelerating and focusing elements are assembled in cryomodules separated by short warm sections. A long open region ({approx} 15 m) allows beam extraction at 1 GeV in support of a nuclear experimental program. In this paper, we present the latest iteration of the CW linac baseline lattice. We also briefly compare it to an alternative where the 162.5 half-wave resonators are replaced with 325 MHz spoke resonators.

  5. Progress on LINAC 4 : Civil engineering (28/07/2009)

    CERN Video Productions

    2009-01-01

    The commissioning of the new Linac4 source – first element of the new acceleration chain for the upgrade of the LHC (sLHC) – has started beginning of July. After years of preparation but after only a few hours of fine-tuning of the numerous parameters involved, the source has delivered its first negative ions.

  6. An Energy Recovery Electron Linac On Ring Collider

    Nikolitsa Merminga; Geoffrey Krafft; Valeri Lebedev; Ilan Ben-Zvi

    2001-09-01

    Electron-proton/ion colliders with center of mass energies between 14 GeV and 100 GeV (protons) or 63 GeV/A (ions) and luminosities at the 10{sup 33} (per nucleon) level have been proposed recently as a means for studying hadronic structure. Electron beam polarization appears to be crucial for many of the experiments. Two accelerator design scenarios have been examined in detail: colliding rings and recirculating linac-on-ring. Although the linac-on-ring scenario is not as well developed as the ring-ring scenario, comparable luminosities appear feasible. The linac-on-ring option presents significant advantages with respect to: (1) spin manipulations; (2) reduction of the synchrotron radiation load in the detectors; (3) a wide range of continuous energy variability. Rf power and beam dump considerations require that the electron linac recover the beam energy. This technology has been demonstrated at Jefferson Lab's IR FEL with cw current up to 5 mA and beam energy up to 50 MeV. Based on extrapolations from actual measurements and calculations, energy recovery is expected to be feasible at higher currents (a few hundred mA) and higher energies (a few GeV) as well. The report begins with a brief overview of Jefferson Lab's experience with energy recovery and summarize its benefits. Luminosity projections for the linac-ring scenario based on fundamental limitations are presented next. The feasibility of an energy recovery electron linac-on-proton ring collider is investigated and four conceptual point designs are shown corresponding to electron to proton energies of: 3 GeV on 15 GeV, 5 GeV on 50 GeV and 10 GeV on 250 GeV, and for gold ions with 100 GeV/A. The last two designs assume that the protons or ions are stored in the existing RHIC accelerator. Accelerator physics issues relevant to proton rings and energy recovery linacs are discussed next and a list of required R and D for the realization of such a design is presented.

  7. Tentative design of beam focusing for the AHF linac and transport systems

    Proposals for an advanced hadron facility include building afterburner linacs for LAMPF. A first afterburner, Add-on Linac number 1, is proposed to accelerate the beam from 0.8 to 1.6 GeV. The output beam would then be fed to a compressor ring and to another afterburner, Add-on Linac number 2. We make a rough estimate of the transverse focusing strength needed in these linacs, and consider the transport line from the end of the LAMPF 805-MHz linac to the start of Add-on Linac number 1. A rebuncher is needed in this transport line for proper acceptance of the beam into the add-on linac. 2 refs., 4 figs

  8. Beam halo in high-intensity hadron linacs

    This document aims to cover the most relevant mechanisms for the development of beam halo in high-intensity hadron linacs. The introduction outlines the various applications of high-intensity linacs and it will explain why, in the case of the CERN Superconducting Proton Linac (SPL) study a linac was chosen to provide a high-power beam, rather than a different kind of accelerator. The basic equations, needed for the understanding of halo development are derived and employed to study the effects of initial and distributed mismatch on high-current beams. The basic concepts of the particle-core model, envelope modes, parametric resonances, the free-energy approach, and the idea of core-core resonances are introduced and extended to study beams in realistic linac lattices. The approach taken is to study the behavior of beams not only in simplified theoretical focusing structures but to highlight the beam dynamics in realistic accelerators. All effects which are described and derived with simplified analytic models, are tested in realistic lattices and are thus related to observable effects in linear accelerators. This approach involves the use of high-performance particle tracking codes, which are needed to simulate the behavior of the outermost particles in distributions of up to 100 million macro particles. In the end a set of design rules are established and their impact on the design of a typical high-intensity machine, the CERN SPL, is shown. The examples given in this document refer to two different design evolutions of the SPL study: the first conceptual design report (SPL I) and the second conceptual design report (SPL II). (orig.)

  9. Beam halo in high-intensity hadron linacs

    Gerigk, F.

    2006-12-21

    This document aims to cover the most relevant mechanisms for the development of beam halo in high-intensity hadron linacs. The introduction outlines the various applications of high-intensity linacs and it will explain why, in the case of the CERN Superconducting Proton Linac (SPL) study a linac was chosen to provide a high-power beam, rather than a different kind of accelerator. The basic equations, needed for the understanding of halo development are derived and employed to study the effects of initial and distributed mismatch on high-current beams. The basic concepts of the particle-core model, envelope modes, parametric resonances, the free-energy approach, and the idea of core-core resonances are introduced and extended to study beams in realistic linac lattices. The approach taken is to study the behavior of beams not only in simplified theoretical focusing structures but to highlight the beam dynamics in realistic accelerators. All effects which are described and derived with simplified analytic models, are tested in realistic lattices and are thus related to observable effects in linear accelerators. This approach involves the use of high-performance particle tracking codes, which are needed to simulate the behavior of the outermost particles in distributions of up to 100 million macro particles. In the end a set of design rules are established and their impact on the design of a typical high-intensity machine, the CERN SPL, is shown. The examples given in this document refer to two different design evolutions of the SPL study: the first conceptual design report (SPL I) and the second conceptual design report (SPL II). (orig.)

  10. Improved performance of the control scheme for IUAC superconducting Linac

    Since many years energized ion beams from linac are being delivered routinely for scheduled experiments using all the three accelerating modules of linac along with super buncher and rebuncher. Major efforts are dedicated to improve the performance of the control scheme to minimise the down time of the linac during operation. Earlier, a number of developments were carried out to improve the dynamics of the control scheme. The most significant of them is the piezoelectric actuator based tuning mechanism which is implemented in all the operational resonators of second and third accelerating modules of superconducting linac. This has helped us to bridge the gap between the accelerating fields achieved during Q measurement at 6 W of helium power and during phase locking of the resonator during beam operation at a given RF power (∼120W). The piezoelectric actuator based tuner is also instrumental to reduce the unlocking rate of the resonators. Pulse width modulation (PWM) control based helium gas operated tuner is implemented in few resonators to improve phase locking performance. CAMAC based distributed control scheme is upgraded to VME based distributed control without changing the existing client interface to maintain uniformity between the Pelletron and linac control. Python code support has been implemented to protect the resonators against high forward power during unlocking. This is also integrated with the display status of the resonators for monitoring. A frequency to voltage converter is incorporated in control scheme to monitor the frequency error. This has helped us to develop a scheme for automatic phase locking of the cavities using piezoelectric actuator based tuner control. (author)

  11. La ciudad lineal del centenario: Los cien años de la utopía lineal/The city's centennial linear: The one hundred years of utopia linear

    Figueroa Salas, Jonás

    2009-06-01

    Full Text Available Desde los primeros años del siglo XX y por algo más de tres décadas, el arquitecto chileno Carlos Carvajal Miranda (1872-1950 presenta proyectos inspirados en las ciudades lineales desarrolladas por Arturo Soria y Mata (1844-1920. Se intenta la resolución de los problemas del crecimiento de la ciudad moderna, de la motorización de los transportes públicos y de la escasa ocupación urbana del país. Es un período rico en manifestaciones públicas y privadas frente a los cambios entre la primera edad republicana del siglo XIX y la temprana modernidad del siglo XX. En términos urbanos se trata de corregir los conflictos que surgen por los cambios socioeconómicos y tecnológicos, y por el interés de conferirle a la ciudad el nivel que ya exhiben otras capitales del continente. Más allá de la posible vigencia que pueden registrar las teorías sobre la ciudad lineal, nos interesa valorar los esfuerzos y la claridad de un arquitecto urbanista para comprometerse con la resolución de los problemas que comienzan a registrase en las ciudades chilenas, echando mano a la modernidad./This article relates to the project architect Carlos Carvajal Miranda (1872-1950, who tries to build linear cities in Chile. Carvajal is inspired by the proposals of the Spanish Soria and Mata, and is committed to solving the problems that are beginning to register in Chilean cities at the beginning of the twentieth century. During this period, attempts to resolve conflicts arising from social, economic and technological change, and give the city a better level as other cities of the continent./

  12. ¿Cuándo la viabilidad implica la estabilidad estructural de un sistema dinámico lineal en tiempo discreto?

    Guzmán, José Ramón; Puchet A., Martín

    1994-01-01

    This paper presents some findings of the theory of control mathematics. These findings are complemented with those referred to viability of lineal dynamic systems on a discrete time period. The purpose of the paper is to establish which conditions should be satisfied by those systems for their viability with structural stability.

  13. Inauguran nuevo tunel de acelerador

    Macedo, C

    2003-01-01

    "Contendra el Gran Colisionador de Hadrones del CERN. Ayer fue inaugurado el tunel subterraneo que acogera al experimento ATLAS, uno de los cuatro xperimentos que integraran el Gran Colisionador de Hadrones (LHC), que es construido en el Centro Europeo para la Investigacion Nuclear (CERN), en Ginebra" (1/3 page).

  14. Calculations of reactivity based in the solution of the Neutron transport equation in X Y geometry and Lineal perturbation theory

    In our country, in last congresses, Gomez et al carried out reactivity calculations based on the solution of the diffusion equation for an energy group using nodal methods in one dimension and the TPL approach (Lineal Perturbation Theory). Later on, Mugica extended the application to the case of multigroup so much so much in one as in two dimensions (X Y geometry) with excellent results. Presently work is carried out similar calculations but this time based on the solution of the neutron transport equation in X Y geometry using nodal methods and again the TPL approximation. The idea is to provide a calculation method that allows to obtain in quick form the reactivity solving the direct problem as well as the enclosed problem of the not perturbed problem. A test problem for the one that results are provided for the effective multiplication factor is described and its are offered some conclusions. (Author)

  15. Performance analysis of the lineal model for estimating the maximum power of a HCPV module in different climate conditions

    Fernández, Eduardo F.; Almonacid, Florencia; Sarmah, Nabin; Mallick, Tapas; Sanchez, Iñigo; Cuadra, Juan M.; Soria-Moya, Alberto; Pérez-Higueras, Pedro

    2014-09-01

    A model based on easily obtained atmospheric parameters and on a simple lineal mathematical expression has been developed at the Centre of Advanced Studies in Energy and Environment in southern Spain. The model predicts the maximum power of a HCPV module as a function of direct normal irradiance, air temperature and air mass. Presently, the proposed model has only been validated in southern Spain and its performance in locations with different atmospheric conditions still remains unknown. In order to address this issue, several HCPV modules have been measured in two different locations with different climate conditions than the south of Spain: the Environment and Sustainability Institute in southern UK and the National Renewable Energy Center in northern Spain. Results show that the model has an adequate match between actual and estimated data with a RMSE lower than 3.9% at locations with different climate conditions.

  16. Sobre el uso de las desigualdades variacionales para el cálculo del problema de complementariedad no lineal.

    Pedreira Andrade, Luis P.

    2003-01-01

    Full Text Available El nacimiento de los problemas de complementariedad no lineal (NCP y de los problemas de desigualdades variacionales (VIP fuertemente ligados a la programación matemática ha dado lugar a numerosos esfuerzos investigadores orientados a resolverlos. En los últimos años ha resultado de vital importancia para la resolución de los VIP el uso de funciones D-gap para reformular el problema como uno de optimización diferenciable sin restricciones. Este artículo pretende ser una presentación de la aplicabilidad de la función D-gap a los NCP con algoritmos recogidos de la literatura, así como un punto de partida para investigaciones que reduzcan las hipótesis para este caso particular.

  17. Nets solution of flow for gases, using the Balance Pattern of Nodes and the method of linealization of equations

    The dimension of nets of distribution of gases is a complex problem, so much for the diversity of the phenomena that they are presented, like for the variation of the properties of the fluids, especially, the density for effect of the changes in the pressure along the net. This work presents a model for its simulation starting from the deduction of the general equation of flow in stable and isothermal state, its inclusion in the pattern of balance of nodes and the solution of this for the method of linealization of equations. Additionally, a summary of the empiric equations more used is made for the calculation of the fall of pressure for gases flowing in pipes and an example that it illustrates the application of the pattern and the developed method

  18. Desarrollo de un Modelo Matemático no Lineal Aplicando Mínimos Cuadrados en un Sistema de Nivel

    Paula A. Ortiz

    2010-06-01

    Full Text Available To perform a system analysis it is necessary to have a mathematical model representing it, which permits simulation of the process dynamics and development of control strategies to be applied in the real system. With this aim, it is important for the model, not being unique, to be a close representation of the process. On this work a non lineal mathematical model is obtained for the level plant at the laboratory of control and measurement of fluidics of the INSTITUTO TECNOLÓGICO METROPOLITANO. Obtaining the model consists of two parts, the first one consists in finding physical equations of the system in terms of some unknown parameters, and the second one consists in finding those parameters using least square method. A validation of the obtained model was made and it was found that the model was reliable. This system identification technique can be applied in other process with known physical equations in terms of unknown parameters.

  19. La fibra óptica y el fenómeno no lineal mezcla de cuarta onda

    Fabián Gómez López

    2015-12-01

    Full Text Available RESUMEN Para aprovechar de mejor manera el ancho de banda que tiene la fibra óptica, los sistemas de comunicaciones ópticos han tenido que aumentar la potencia de transmisión de las señales para poder transportar a grandes distancias la información. Debido a lo anterior, comienzan a producirse ciertos fenómenos ópticos no lineales como la mezcla de cuarta onda (Four Wave Mixing, FWM, que degradan la señal de información. En este documento se realiza un estado del arte de la fibra óptica y un estudio del fenómeno no lineal FWM, que se genera cuando dos o más señales ópticas se propagan en la fibra, lo cual conlleva a una mezcla de señales que puede generar nuevos componentes de interferencia de la señal óptica transmitida. ABSTRACT To make better use of the bandwidth that has the optical fiber, optical communications systems have had to increase the transmission power of signals to transport information over long distances. Because of this, certain nonlinear optical phenomena such as four wave mixing (Four Wave Mixing, FWM, which degrade the information signal begin to occur. Herein a state of the art of optical fiber and a study of the nonlinear FWM phenomenon, which is generated when two or more optical signals propagating in the fiber takes place, which leads to a mixture of signals that can generate new components interference of the transmitted optical signal.

  20. The main linac cavity for Cornell's energy recovery linac: Cavity design through horizontal cryomodule prototype test

    Future particle accelerators will require continuous wave operation of SRF cavities capable of supporting high beam currents. An example of this is the Energy Recovery Linac (ERL) at Cornell University, a next generation light source designed to run high currents (100 mA) with a high bunch repetition rate (1.3 GHz). Obtaining the beam emittance necessary to meet design specification requires strong damping of higher-order modes that can lead to beam breakup. We discuss the optimization and verification of the accelerating cavity. Next we show that an ERL constructed from the optimized cavity geometry – including realistic shape errors – can support beam currents in excess of 300 mA while still maintaining beam stability. A niobium prototype 7-cell cavity was fabricated and tested in a horizontal cryomodule. We show that the prototype cavity exceeds quality factor and gradient specifications of 2×1010 at 16.2 MV/m at 1.8 K by 50%, reaching Q=(3.0±0.3)×1010. The prototype cavity also satisfies all design constraints and has a higher order mode spectrum consistent with the optimized shape geometry. At 1.6 K, the cavity set a record for quality factor of a multicell cavity installed in a horizontal cryomodule reaching Q=(6.1±0.6)×1010