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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...

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Detalles Bibliográficos
Autores principales: Berg, J S, Ruggiero, F
Lenguaje:eng
Publicado: 1997
Materias:
Acceso en línea:http://cds.cern.ch/record/328011
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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
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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
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