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Measurements with a Novel Non-Intercepting Bunch Shape Monitor at the High Current GSI-LINAC

For bunch length determination in the range of 0.3 to 5 ns at the GSI heavy ion LINAC a novel, non-intercepting device has been realized. It uses the time spectrum of secondary electrons created by atomic collisions between beam ions and residual gas molecules. These electrons are accelerated by an...

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Detalles Bibliográficos
Autores principales: Forck, P, Dorn, C
Lenguaje:eng
Publicado: 2005
Materias:
Acceso en línea:http://cds.cern.ch/record/924198
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author Forck, P
Dorn, C
author_facet Forck, P
Dorn, C
author_sort Forck, P
collection CERN
description For bunch length determination in the range of 0.3 to 5 ns at the GSI heavy ion LINAC a novel, non-intercepting device has been realized. It uses the time spectrum of secondary electrons created by atomic collisions between beam ions and residual gas molecules. These electrons are accelerated by an electric field of 400 V/mm toward an electro-static energy analyzer, which is used to restrict the effective source region. Then the electrons are deflected by an rf-resonator running in phase with the acceleration frequency (36 or 108 MHz) to transform the time spectrum into spatial separation. The detection is done with a multi-channel plate equipped with a phosphor screen and observed by a CCD camera. The achieved time resolution is about 60 ps, corresponding to 2 degree of 108 MHz. The general layout of the device and first results will be presented.
id cern-924198
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2005
record_format invenio
spelling cern-9241982019-09-30T06:29:59Zhttp://cds.cern.ch/record/924198engForck, PDorn, CMeasurements with a Novel Non-Intercepting Bunch Shape Monitor at the High Current GSI-LINACAccelerators and Storage RingsFor bunch length determination in the range of 0.3 to 5 ns at the GSI heavy ion LINAC a novel, non-intercepting device has been realized. It uses the time spectrum of secondary electrons created by atomic collisions between beam ions and residual gas molecules. These electrons are accelerated by an electric field of 400 V/mm toward an electro-static energy analyzer, which is used to restrict the effective source region. Then the electrons are deflected by an rf-resonator running in phase with the acceleration frequency (36 or 108 MHz) to transform the time spectrum into spatial separation. The detection is done with a multi-channel plate equipped with a phosphor screen and observed by a CCD camera. The achieved time resolution is about 60 ps, corresponding to 2 degree of 108 MHz. The general layout of the device and first results will be presented.CARE-CONF-05-028-HIPPICARE-CONF-2005-028-HIPPIoai:cds.cern.ch:9241982005
spellingShingle Accelerators and Storage Rings
Forck, P
Dorn, C
Measurements with a Novel Non-Intercepting Bunch Shape Monitor at the High Current GSI-LINAC
title Measurements with a Novel Non-Intercepting Bunch Shape Monitor at the High Current GSI-LINAC
title_full Measurements with a Novel Non-Intercepting Bunch Shape Monitor at the High Current GSI-LINAC
title_fullStr Measurements with a Novel Non-Intercepting Bunch Shape Monitor at the High Current GSI-LINAC
title_full_unstemmed Measurements with a Novel Non-Intercepting Bunch Shape Monitor at the High Current GSI-LINAC
title_short Measurements with a Novel Non-Intercepting Bunch Shape Monitor at the High Current GSI-LINAC
title_sort measurements with a novel non-intercepting bunch shape monitor at the high current gsi-linac
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/924198
work_keys_str_mv AT forckp measurementswithanovelnoninterceptingbunchshapemonitoratthehighcurrentgsilinac
AT dornc measurementswithanovelnoninterceptingbunchshapemonitoratthehighcurrentgsilinac