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Stochastic cooling of bunched ions simulated in the time domain
To include the influence of synchrotron oscillations, beam feedback and IBS a particle by particle and turn by turn treatment in the time-domain has been tried out. – Complete pickup, amplification and kicker characteristics, defined in the frequency domain, are introduced via inverse Laplace t...
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Lenguaje: | eng |
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2013
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Acceso en línea: | http://cds.cern.ch/record/1704333 |
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author | Thorndahl, L |
author_facet | Thorndahl, L |
author_sort | Thorndahl, L |
collection | CERN |
description | To include the influence of synchrotron oscillations, beam feedback and IBS a particle by particle and turn by turn treatment in the time-domain has been tried out. – Complete pickup, amplification and kicker characteristics, defined in the frequency domain, are introduced via inverse Laplace transformation, and so is the Dirac function representing the single ion. – The computation time is kept within reasonable limits thanks to the rule that cooling times scale proportionally with the particle number [1]. Typically 10000 simulation particles are cooled in 1200 turns. A recent proposal [2], based on signal binning and FFTs, offers the potential for at least one order of magnitude more ions and turns. |
id | cern-1704333 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2013 |
record_format | invenio |
spelling | cern-17043332019-09-30T06:29:59Zhttp://cds.cern.ch/record/1704333engThorndahl, LStochastic cooling of bunched ions simulated in the time domainAccelerators and Storage RingsTo include the influence of synchrotron oscillations, beam feedback and IBS a particle by particle and turn by turn treatment in the time-domain has been tried out. – Complete pickup, amplification and kicker characteristics, defined in the frequency domain, are introduced via inverse Laplace transformation, and so is the Dirac function representing the single ion. – The computation time is kept within reasonable limits thanks to the rule that cooling times scale proportionally with the particle number [1]. Typically 10000 simulation particles are cooled in 1200 turns. A recent proposal [2], based on signal binning and FFTs, offers the potential for at least one order of magnitude more ions and turns.oai:cds.cern.ch:17043332013 |
spellingShingle | Accelerators and Storage Rings Thorndahl, L Stochastic cooling of bunched ions simulated in the time domain |
title | Stochastic cooling of bunched ions simulated in the time domain |
title_full | Stochastic cooling of bunched ions simulated in the time domain |
title_fullStr | Stochastic cooling of bunched ions simulated in the time domain |
title_full_unstemmed | Stochastic cooling of bunched ions simulated in the time domain |
title_short | Stochastic cooling of bunched ions simulated in the time domain |
title_sort | stochastic cooling of bunched ions simulated in the time domain |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/1704333 |
work_keys_str_mv | AT thorndahll stochasticcoolingofbunchedionssimulatedinthetimedomain |