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Beam dynamic simulation and optimization of the CLIC positron source and the capture linac
The CLIC Positron Source is based on the hybrid target composed of a crystal and an amorphous target. Simulations have been performed from the exit of the amorphous target to the end of pre-injector linac which captures and accelerates the positrons to an energy of 200 MeV. Simulations are performed...
Autores principales: | , , |
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Lenguaje: | eng |
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2016
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1063/1.4944155 http://cds.cern.ch/record/2263089 |
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author | Bayar, C Doebert, S Ciftci, A K |
author_facet | Bayar, C Doebert, S Ciftci, A K |
author_sort | Bayar, C |
collection | CERN |
description | The CLIC Positron Source is based on the hybrid target composed of a crystal and an amorphous target. Simulations have been performed from the exit of the amorphous target to the end of pre-injector linac which captures and accelerates the positrons to an energy of 200 MeV. Simulations are performed by the particle tracking code PARMELA. The magnetic field of the AMD is represented in PARMELA by simple coils. Two modes are applied in this study. The first one is accelerating mode based on acceleration after the AMD. The second one is decelerating mode based on deceleration in the first accelerating structure. It is shown that the decelerating mode gives a higher yield for the e+beam in the end of the Pre-Injector Linac. |
id | oai-inspirehep.net-1439287 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2016 |
record_format | invenio |
spelling | oai-inspirehep.net-14392872019-09-30T06:29:59Zdoi:10.1063/1.4944155http://cds.cern.ch/record/2263089engBayar, CDoebert, SCiftci, A KBeam dynamic simulation and optimization of the CLIC positron source and the capture linacAccelerators and Storage RingsThe CLIC Positron Source is based on the hybrid target composed of a crystal and an amorphous target. Simulations have been performed from the exit of the amorphous target to the end of pre-injector linac which captures and accelerates the positrons to an energy of 200 MeV. Simulations are performed by the particle tracking code PARMELA. The magnetic field of the AMD is represented in PARMELA by simple coils. Two modes are applied in this study. The first one is accelerating mode based on acceleration after the AMD. The second one is decelerating mode based on deceleration in the first accelerating structure. It is shown that the decelerating mode gives a higher yield for the e+beam in the end of the Pre-Injector Linac.oai:inspirehep.net:14392872016 |
spellingShingle | Accelerators and Storage Rings Bayar, C Doebert, S Ciftci, A K Beam dynamic simulation and optimization of the CLIC positron source and the capture linac |
title | Beam dynamic simulation and optimization of the CLIC positron source and the capture linac |
title_full | Beam dynamic simulation and optimization of the CLIC positron source and the capture linac |
title_fullStr | Beam dynamic simulation and optimization of the CLIC positron source and the capture linac |
title_full_unstemmed | Beam dynamic simulation and optimization of the CLIC positron source and the capture linac |
title_short | Beam dynamic simulation and optimization of the CLIC positron source and the capture linac |
title_sort | beam dynamic simulation and optimization of the clic positron source and the capture linac |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.1063/1.4944155 http://cds.cern.ch/record/2263089 |
work_keys_str_mv | AT bayarc beamdynamicsimulationandoptimizationoftheclicpositronsourceandthecapturelinac AT doeberts beamdynamicsimulationandoptimizationoftheclicpositronsourceandthecapturelinac AT ciftciak beamdynamicsimulationandoptimizationoftheclicpositronsourceandthecapturelinac |