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The CLIC electron and positron polarized sources
The CLIC polarized electron source is based on a DC gun where the photocathode is illuminated by a laser beam. Each micro-bunch has a charge of 6x109 e−, a width of 100 ps and a repetition rate of 2 GHz. A peak current of 10 A in the micro-bunch is a challenge for the surface charge limit of the pho...
Autores principales: | , , , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
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2010
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/1269911 |
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author | Rinolfi, Louis Brachmann, Axel Bulyak, Eugene Chehab, Robert Dadoun, Olivier Gai, Wei Gladkikh, Peter Kamitani, Takuya Kuriki, Masao Liu, Wanming Maryuama, Takashi Omori, Tsunehiko Poelker, Matt Sheppard, John Urakawa, Junji Variola, Alessandro Vivoli, Alessandro Yakimenko, Vitaly Zhou, Feng Zimmermann, Frank |
author_facet | Rinolfi, Louis Brachmann, Axel Bulyak, Eugene Chehab, Robert Dadoun, Olivier Gai, Wei Gladkikh, Peter Kamitani, Takuya Kuriki, Masao Liu, Wanming Maryuama, Takashi Omori, Tsunehiko Poelker, Matt Sheppard, John Urakawa, Junji Variola, Alessandro Vivoli, Alessandro Yakimenko, Vitaly Zhou, Feng Zimmermann, Frank |
author_sort | Rinolfi, Louis |
collection | CERN |
description | The CLIC polarized electron source is based on a DC gun where the photocathode is illuminated by a laser beam. Each micro-bunch has a charge of 6x109 e−, a width of 100 ps and a repetition rate of 2 GHz. A peak current of 10 A in the micro-bunch is a challenge for the surface charge limit of the photo-cathode. Two options are feasible to generate the 2 GHz e− bunch train: 100 ps micro-bunches can be extracted from the photo-cathode either by a 2 GHz laser system or by generating a macro-bunch using a ~200 ns laser pulse and a subsequent RF bunching system to produce the appropriate micro-bunch structure. Recent results obtained by SLAC, for the latter case, are presented. The polarized positron source is based on a positron production scheme in which polarized photons are produced by a laser Compton scattering process. The resulting circularly-polarized gamma photons are sent onto a target, producing pairs of longitudinally polarized electrons and positrons. The Compton backscattering process occurs either in a Compton ring, where a 1 GeV electron beam interacts with circularly-polarized photons in an optical resonator or in a 1.8 GeV Compton Energy Recovery Linac (ERL) or in a 6 GeV Linac with several optical cavities. The undulator scheme is also studied. The nominal CLIC e+ bunch population is 6.7x109 particles per bunch at 200 MeV. The tradeoff between e+ yield and level of polarization is an important topic. The overal l scheme for both polarized electron and positron beams is described. |
id | cern-1269911 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2010 |
record_format | invenio |
spelling | cern-12699112023-07-20T15:01:27Zhttp://cds.cern.ch/record/1269911engRinolfi, LouisBrachmann, AxelBulyak, EugeneChehab, RobertDadoun, OlivierGai, WeiGladkikh, PeterKamitani, TakuyaKuriki, MasaoLiu, WanmingMaryuama, TakashiOmori, TsunehikoPoelker, MattSheppard, JohnUrakawa, JunjiVariola, AlessandroVivoli, AlessandroYakimenko, VitalyZhou, FengZimmermann, FrankThe CLIC electron and positron polarized sourcesAccelerators and Storage RingsThe CLIC polarized electron source is based on a DC gun where the photocathode is illuminated by a laser beam. Each micro-bunch has a charge of 6x109 e−, a width of 100 ps and a repetition rate of 2 GHz. A peak current of 10 A in the micro-bunch is a challenge for the surface charge limit of the photo-cathode. Two options are feasible to generate the 2 GHz e− bunch train: 100 ps micro-bunches can be extracted from the photo-cathode either by a 2 GHz laser system or by generating a macro-bunch using a ~200 ns laser pulse and a subsequent RF bunching system to produce the appropriate micro-bunch structure. Recent results obtained by SLAC, for the latter case, are presented. The polarized positron source is based on a positron production scheme in which polarized photons are produced by a laser Compton scattering process. The resulting circularly-polarized gamma photons are sent onto a target, producing pairs of longitudinally polarized electrons and positrons. The Compton backscattering process occurs either in a Compton ring, where a 1 GeV electron beam interacts with circularly-polarized photons in an optical resonator or in a 1.8 GeV Compton Energy Recovery Linac (ERL) or in a 6 GeV Linac with several optical cavities. The undulator scheme is also studied. The nominal CLIC e+ bunch population is 6.7x109 particles per bunch at 200 MeV. The tradeoff between e+ yield and level of polarization is an important topic. The overal l scheme for both polarized electron and positron beams is described.CERN-OPEN-2010-017CLIC-Note-817oai:cds.cern.ch:12699112010-01-08 |
spellingShingle | Accelerators and Storage Rings Rinolfi, Louis Brachmann, Axel Bulyak, Eugene Chehab, Robert Dadoun, Olivier Gai, Wei Gladkikh, Peter Kamitani, Takuya Kuriki, Masao Liu, Wanming Maryuama, Takashi Omori, Tsunehiko Poelker, Matt Sheppard, John Urakawa, Junji Variola, Alessandro Vivoli, Alessandro Yakimenko, Vitaly Zhou, Feng Zimmermann, Frank The CLIC electron and positron polarized sources |
title | The CLIC electron and positron polarized sources |
title_full | The CLIC electron and positron polarized sources |
title_fullStr | The CLIC electron and positron polarized sources |
title_full_unstemmed | The CLIC electron and positron polarized sources |
title_short | The CLIC electron and positron polarized sources |
title_sort | clic electron and positron polarized sources |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/1269911 |
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