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Stability diagrams for Landau damping
Coherent modes which are present when there is no incoherent tune spread may be absent when such a spread exists. Such modes are``Landau damped.'' There is instead an incoherent spectrum, a continuum of an infinite number of frequencies, which will decohere (filament), thus not leading to...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
1997
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Acceso en línea: | http://cds.cern.ch/record/328011 |
_version_ | 1780891003397341184 |
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author | Berg, J S Ruggiero, F |
author_facet | Berg, J S Ruggiero, F |
author_sort | Berg, J S |
collection | CERN |
description | Coherent modes which are present when there is no incoherent tune spread may be absent when such a spread exists. Such modes are``Landau damped.'' There is instead an incoherent spectrum, a continuum of an infinite number of frequencies, which will decohere (filament), thus not leading to collective instabilities. A stability diagram indicates when Landau damping will be effective. It divides the effective impedance plane, or equivalently the plane of coherent frequency in the absence of tune spread, into regions. The region which contains +i/infinity corresponds to instability. Thus, one can substitute a simpler computation (finding discrete eigenvalues) for a more complex computation (solving an eigenvalue system with both a discrete and a continuous eigenvalue spectrum). We present stability diagrams assuming a linear tune shift with amplitude, allowing tune spread in two transverse planes or in the longitudinal plane alone. When there is longitudinal tune spread, this can not be done exactly, and we describe approximations which make the computation tractable. |
id | cern-328011 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1997 |
record_format | invenio |
spelling | cern-3280112023-05-31T13:21:20Zhttp://cds.cern.ch/record/328011engBerg, J SRuggiero, FStability diagrams for Landau dampingAccelerators and Storage RingsCoherent modes which are present when there is no incoherent tune spread may be absent when such a spread exists. Such modes are``Landau damped.'' There is instead an incoherent spectrum, a continuum of an infinite number of frequencies, which will decohere (filament), thus not leading to collective instabilities. A stability diagram indicates when Landau damping will be effective. It divides the effective impedance plane, or equivalently the plane of coherent frequency in the absence of tune spread, into regions. The region which contains +i/infinity corresponds to instability. Thus, one can substitute a simpler computation (finding discrete eigenvalues) for a more complex computation (solving an eigenvalue system with both a discrete and a continuous eigenvalue spectrum). We present stability diagrams assuming a linear tune shift with amplitude, allowing tune spread in two transverse planes or in the longitudinal plane alone. When there is longitudinal tune spread, this can not be done exactly, and we describe approximations which make the computation tractable.LHC-Project-Report-121CERN-LHC-Project-Report-121oai:cds.cern.ch:3280111997-06-11 |
spellingShingle | Accelerators and Storage Rings Berg, J S Ruggiero, F Stability diagrams for Landau damping |
title | Stability diagrams for Landau damping |
title_full | Stability diagrams for Landau damping |
title_fullStr | Stability diagrams for Landau damping |
title_full_unstemmed | Stability diagrams for Landau damping |
title_short | Stability diagrams for Landau damping |
title_sort | stability diagrams for landau damping |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/328011 |
work_keys_str_mv | AT bergjs stabilitydiagramsforlandaudamping AT ruggierof stabilitydiagramsforlandaudamping |