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Low level RF systems for synchrotrons Part 1: Low intensity case

The low level RF system generates the drive sent to the high power equipment. It uses signals from the main bending magnet (B field) and from beam pick-ups (radial and longitudinal positions). It must minimise the beam losses and provide a beam with reproducible parameters (intensity, bunch length,...

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Detalles Bibliográficos
Autor principal: Baudrenghien, P
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:http://cds.cern.ch/record/702642
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author Baudrenghien, P
author_facet Baudrenghien, P
author_sort Baudrenghien, P
collection CERN
description The low level RF system generates the drive sent to the high power equipment. It uses signals from the main bending magnet (B field) and from beam pick-ups (radial and longitudinal positions). It must minimise the beam losses and provide a beam with reproducible parameters (intensity, bunch length, average momentum and momentum spread) to either the next accelerator or the physicists. This presentation is the first of two parts: It considers the low intensity case where the voltage in the RF cavity is not influenced by the beam. The feedback loops that do not include the beam (accelerating field amplitude and cavity tuning) will not be presented.
id cern-702642
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2001
record_format invenio
spelling cern-7026422023-05-11T12:03:32Zhttp://cds.cern.ch/record/702642engBaudrenghien, PLow level RF systems for synchrotrons Part 1: Low intensity caseAccelerators and Storage RingsThe low level RF system generates the drive sent to the high power equipment. It uses signals from the main bending magnet (B field) and from beam pick-ups (radial and longitudinal positions). It must minimise the beam losses and provide a beam with reproducible parameters (intensity, bunch length, average momentum and momentum spread) to either the next accelerator or the physicists. This presentation is the first of two parts: It considers the low intensity case where the voltage in the RF cavity is not influenced by the beam. The feedback loops that do not include the beam (accelerating field amplitude and cavity tuning) will not be presented.SL-Note-2001-008-HRFoai:cds.cern.ch:7026422001-03-02
spellingShingle Accelerators and Storage Rings
Baudrenghien, P
Low level RF systems for synchrotrons Part 1: Low intensity case
title Low level RF systems for synchrotrons Part 1: Low intensity case
title_full Low level RF systems for synchrotrons Part 1: Low intensity case
title_fullStr Low level RF systems for synchrotrons Part 1: Low intensity case
title_full_unstemmed Low level RF systems for synchrotrons Part 1: Low intensity case
title_short Low level RF systems for synchrotrons Part 1: Low intensity case
title_sort low level rf systems for synchrotrons part 1: low intensity case
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/702642
work_keys_str_mv AT baudrenghienp lowlevelrfsystemsforsynchrotronspart1lowintensitycase