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Automated injection procedure for the CERN intersecting storage rings (ISR)

The performance of the ISR is critically dependent on the conservation of the transverse beam size. One important source of transverse blow- up for proton beams is injection errors. A two-phase injection procedure is designed to limit these errors to negligible proportions. The first phase, based on...

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Detalles Bibliográficos
Autor principal: Vos, L
Lenguaje:eng
Publicado: 1981
Materias:
Acceso en línea:https://dx.doi.org/10.1109/TNS.1981.4331998
http://cds.cern.ch/record/878249
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author Vos, L
author_facet Vos, L
author_sort Vos, L
collection CERN
description The performance of the ISR is critically dependent on the conservation of the transverse beam size. One important source of transverse blow- up for proton beams is injection errors. A two-phase injection procedure is designed to limit these errors to negligible proportions. The first phase, based on the analysis of the first turn beam trajectory, reduces the errors sufficiently to ensure that nearly all of the particles ejected by the CERN-PS will circulate on the ISR injection orbit. The remaining errors are reduced in a second phase based on the accurate measurement of the injection error amplitude, i.e. the amplitude of the coherent betatron oscillation of the injected beam. The residual error causes a blow-up not exceeding a few per cent. The two phases are fully automated using the ISR control computer. (5 refs).
id cern-878249
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1981
record_format invenio
spelling cern-8782492019-09-30T06:29:59Zdoi:10.1109/TNS.1981.4331998http://cds.cern.ch/record/878249engVos, LAutomated injection procedure for the CERN intersecting storage rings (ISR)Nuclear PhysicsThe performance of the ISR is critically dependent on the conservation of the transverse beam size. One important source of transverse blow- up for proton beams is injection errors. A two-phase injection procedure is designed to limit these errors to negligible proportions. The first phase, based on the analysis of the first turn beam trajectory, reduces the errors sufficiently to ensure that nearly all of the particles ejected by the CERN-PS will circulate on the ISR injection orbit. The remaining errors are reduced in a second phase based on the accurate measurement of the injection error amplitude, i.e. the amplitude of the coherent betatron oscillation of the injected beam. The residual error causes a blow-up not exceeding a few per cent. The two phases are fully automated using the ISR control computer. (5 refs).oai:cds.cern.ch:8782491981
spellingShingle Nuclear Physics
Vos, L
Automated injection procedure for the CERN intersecting storage rings (ISR)
title Automated injection procedure for the CERN intersecting storage rings (ISR)
title_full Automated injection procedure for the CERN intersecting storage rings (ISR)
title_fullStr Automated injection procedure for the CERN intersecting storage rings (ISR)
title_full_unstemmed Automated injection procedure for the CERN intersecting storage rings (ISR)
title_short Automated injection procedure for the CERN intersecting storage rings (ISR)
title_sort automated injection procedure for the cern intersecting storage rings (isr)
topic Nuclear Physics
url https://dx.doi.org/10.1109/TNS.1981.4331998
http://cds.cern.ch/record/878249
work_keys_str_mv AT vosl automatedinjectionprocedureforthecernintersectingstorageringsisr