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Compensation of beam loading in the ISR RF cavities

The RF cavities employed for stacking in the ISR are equipped with a powerful feedback system, which compensates for most the beam-induced voltage. This system is, however, limited-mainly by the current in the final amplifier tube-to injected beam intensities of about 5*10/sup 12 / protons at most....

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Detalles Bibliográficos
Autores principales: Frischholz, Hans, Schnell, Wolfgang
Lenguaje:eng
Publicado: 1977
Materias:
Acceso en línea:https://dx.doi.org/10.1109/TNS.1977.4329051
http://cds.cern.ch/record/878549
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author Frischholz, Hans
Schnell, Wolfgang
author_facet Frischholz, Hans
Schnell, Wolfgang
author_sort Frischholz, Hans
collection CERN
description The RF cavities employed for stacking in the ISR are equipped with a powerful feedback system, which compensates for most the beam-induced voltage. This system is, however, limited-mainly by the current in the final amplifier tube-to injected beam intensities of about 5*10/sup 12 / protons at most. Higher intensities are now available from the PS. Additional beam-load compensation has, therefore, been added to the existing cavities and feedback amplifiers. This beam-load compensation consists of a pick-up, a one-turn delay cable, a wide-band amplifier chain and a final amplifier, directly connected to the accelerating gap. This system injects into the cavity a current approximately equal and opposite to the beam current. (3 refs).
id cern-878549
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1977
record_format invenio
spelling cern-8785492023-05-17T13:46:52Zdoi:10.1109/TNS.1977.4329051http://cds.cern.ch/record/878549engFrischholz, HansSchnell, WolfgangCompensation of beam loading in the ISR RF cavitiesNuclear PhysicsThe RF cavities employed for stacking in the ISR are equipped with a powerful feedback system, which compensates for most the beam-induced voltage. This system is, however, limited-mainly by the current in the final amplifier tube-to injected beam intensities of about 5*10/sup 12 / protons at most. Higher intensities are now available from the PS. Additional beam-load compensation has, therefore, been added to the existing cavities and feedback amplifiers. This beam-load compensation consists of a pick-up, a one-turn delay cable, a wide-band amplifier chain and a final amplifier, directly connected to the accelerating gap. This system injects into the cavity a current approximately equal and opposite to the beam current. (3 refs).CERN-ISR-RF-77-11oai:cds.cern.ch:8785491977
spellingShingle Nuclear Physics
Frischholz, Hans
Schnell, Wolfgang
Compensation of beam loading in the ISR RF cavities
title Compensation of beam loading in the ISR RF cavities
title_full Compensation of beam loading in the ISR RF cavities
title_fullStr Compensation of beam loading in the ISR RF cavities
title_full_unstemmed Compensation of beam loading in the ISR RF cavities
title_short Compensation of beam loading in the ISR RF cavities
title_sort compensation of beam loading in the isr rf cavities
topic Nuclear Physics
url https://dx.doi.org/10.1109/TNS.1977.4329051
http://cds.cern.ch/record/878549
work_keys_str_mv AT frischholzhans compensationofbeamloadingintheisrrfcavities
AT schnellwolfgang compensationofbeamloadingintheisrrfcavities