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The 50 MHz transverse feedback system in the CERN ISR
One of the intensity limits in the ISR is imposed by the transverse coherent instability. The intensity at which the instability occurs may be raised by Landau damping, i.e. increasing the tune spread of the stacked beam. However, due to nonlinear resonances, the maximum tune spread is limited. A 50...
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.1977.4329103 http://cds.cern.ch/record/878548 |
_version_ | 1780907994005897216 |
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author | Carron, G Myers, S Thorndahl, L |
author_facet | Carron, G Myers, S Thorndahl, L |
author_sort | Carron, G |
collection | CERN |
description | One of the intensity limits in the ISR is imposed by the transverse coherent instability. The intensity at which the instability occurs may be raised by Landau damping, i.e. increasing the tune spread of the stacked beam. However, due to nonlinear resonances, the maximum tune spread is limited. A 50 MHz feedback system has now been installed which damps the first 166 modes of the instability. Hence at low chromaticity values the critical intensity is raised by around another factor of two. The electronic gain of this system decreases with frequency in order to limit the blow-up of vertical oscillations due to electronic noise and to reduce phase errors at high frequencies. The 50 MHz system has been used to explore the ISR vacuum limit to intensities of 39 A. |
id | cern-878548 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1977 |
record_format | invenio |
spelling | cern-8785482023-04-21T09:45:10Zdoi:10.1109/TNS.1977.4329103http://cds.cern.ch/record/878548engCarron, GMyers, SThorndahl, LThe 50 MHz transverse feedback system in the CERN ISRAccelerators and Storage RingsOne of the intensity limits in the ISR is imposed by the transverse coherent instability. The intensity at which the instability occurs may be raised by Landau damping, i.e. increasing the tune spread of the stacked beam. However, due to nonlinear resonances, the maximum tune spread is limited. A 50 MHz feedback system has now been installed which damps the first 166 modes of the instability. Hence at low chromaticity values the critical intensity is raised by around another factor of two. The electronic gain of this system decreases with frequency in order to limit the blow-up of vertical oscillations due to electronic noise and to reduce phase errors at high frequencies. The 50 MHz system has been used to explore the ISR vacuum limit to intensities of 39 A.CERN-ISR-OP-RF-77-15ISR-OP-RF-77-15oai:cds.cern.ch:8785481977 |
spellingShingle | Accelerators and Storage Rings Carron, G Myers, S Thorndahl, L The 50 MHz transverse feedback system in the CERN ISR |
title | The 50 MHz transverse feedback system in the CERN ISR |
title_full | The 50 MHz transverse feedback system in the CERN ISR |
title_fullStr | The 50 MHz transverse feedback system in the CERN ISR |
title_full_unstemmed | The 50 MHz transverse feedback system in the CERN ISR |
title_short | The 50 MHz transverse feedback system in the CERN ISR |
title_sort | 50 mhz transverse feedback system in the cern isr |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.1109/TNS.1977.4329103 http://cds.cern.ch/record/878548 |
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