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A Z Factory in the VLLC Injector

A Z factory in the VLLC injector with polarized beams is presented. Its circumference is about two Tevatron circumferences. Wigglers make the bunches longer at injection, and reduce the risk of collective instabilities and the polarization time at collision energy. However, they are powerful sources...

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Autor principal: Keil, Eberhard
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:http://cds.cern.ch/record/500823
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author Keil, Eberhard
author_facet Keil, Eberhard
author_sort Keil, Eberhard
collection CERN
description A Z factory in the VLLC injector with polarized beams is presented. Its circumference is about two Tevatron circumferences. Wigglers make the bunches longer at injection, and reduce the risk of collective instabilities and the polarization time at collision energy. However, they are powerful sources of synchrotron radiation, and associated damage. The vertical amplitude function beta_y^* at the interaction point is assumed to be 40 mm. At this value, reaching a peak luminosity 10^33cm^-2s^-1 implies about 50 MW of RF power for the two beams. A lower value of beta_y^* could be exploited by using any intermediate method between two extremes: (i) At constant L and RF power, the circumference and the polarization time could be reduced. (ii) At constant circumference, RF power, and polarization time, L could be increased. Apertures and separation schemes have only been designed at the collision energy. In the discussion of polarization time, peak polarization and figure of merit, all depolarizing mechanisms, due to the momentum spread in the beam and orbit errors, are ignored.
id cern-500823
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2001
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spelling cern-5008232023-05-05T13:08:01Zhttp://cds.cern.ch/record/500823engKeil, EberhardA Z Factory in the VLLC InjectorAccelerators and Storage RingsA Z factory in the VLLC injector with polarized beams is presented. Its circumference is about two Tevatron circumferences. Wigglers make the bunches longer at injection, and reduce the risk of collective instabilities and the polarization time at collision energy. However, they are powerful sources of synchrotron radiation, and associated damage. The vertical amplitude function beta_y^* at the interaction point is assumed to be 40 mm. At this value, reaching a peak luminosity 10^33cm^-2s^-1 implies about 50 MW of RF power for the two beams. A lower value of beta_y^* could be exploited by using any intermediate method between two extremes: (i) At constant L and RF power, the circumference and the polarization time could be reduced. (ii) At constant circumference, RF power, and polarization time, L could be increased. Apertures and separation schemes have only been designed at the collision energy. In the discussion of polarization time, peak polarization and figure of merit, all depolarizing mechanisms, due to the momentum spread in the beam and orbit errors, are ignored.CERN-SL-2001-013-APoai:cds.cern.ch:5008232001-05-22
spellingShingle Accelerators and Storage Rings
Keil, Eberhard
A Z Factory in the VLLC Injector
title A Z Factory in the VLLC Injector
title_full A Z Factory in the VLLC Injector
title_fullStr A Z Factory in the VLLC Injector
title_full_unstemmed A Z Factory in the VLLC Injector
title_short A Z Factory in the VLLC Injector
title_sort z factory in the vllc injector
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/500823
work_keys_str_mv AT keileberhard azfactoryinthevllcinjector
AT keileberhard zfactoryinthevllcinjector