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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....
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
1977
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1109/TNS.1977.4329051 http://cds.cern.ch/record/878549 |
_version_ | 1780907994217709568 |
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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 |