Practical method for measurement and compensation of linear coupling driving term

We demonstrated a method with practical value for the measurement and global compensation of a complex coupling driving term C of linear difference resonance, using a turn-by-turn beam position monitor (BPM) at the SPring-8 storage ring. The method is based on the perturbation theory with the single...

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Main Authors: M. Masaki, M. Takao, K. Soutome, S. Takano
Format: Article
Language:English
Published: American Physical Society 2009-02-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.12.024002
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spelling doaj-a49b64ac504849e0adb785b52ebcf50a2020-11-24T21:31:45ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022009-02-0112202400210.1103/PhysRevSTAB.12.024002Practical method for measurement and compensation of linear coupling driving termM. MasakiM. TakaoK. SoutomeS. TakanoWe demonstrated a method with practical value for the measurement and global compensation of a complex coupling driving term C of linear difference resonance, using a turn-by-turn beam position monitor (BPM) at the SPring-8 storage ring. The method is based on the perturbation theory with the single-resonance approximation. The accurate complex C was obtained from coefficients of the eigenmode expansion of the coupled betatron oscillation observed near a target linear difference resonance. The global compensation for the measured C was successfully carried out by determining optimal strengths of the two independent correcting skew quadrupoles for generating a counterterm -C without using empirical methods. Meanwhile, we then confirmed that the determined optimal strengths gave a minimum vertical beam size by scanning the strength of the correcting skew quadrupole field. To demonstrate the validity of our method, C was also measured while varying the strengths of the correcting magnets around the optimal values to generate deliberate skew quadrupole error fields. We confirmed that the measured values of C agreed with those coming from the deliberate error fields.http://doi.org/10.1103/PhysRevSTAB.12.024002
collection DOAJ
language English
format Article
sources DOAJ
author M. Masaki
M. Takao
K. Soutome
S. Takano
spellingShingle M. Masaki
M. Takao
K. Soutome
S. Takano
Practical method for measurement and compensation of linear coupling driving term
Physical Review Special Topics. Accelerators and Beams
author_facet M. Masaki
M. Takao
K. Soutome
S. Takano
author_sort M. Masaki
title Practical method for measurement and compensation of linear coupling driving term
title_short Practical method for measurement and compensation of linear coupling driving term
title_full Practical method for measurement and compensation of linear coupling driving term
title_fullStr Practical method for measurement and compensation of linear coupling driving term
title_full_unstemmed Practical method for measurement and compensation of linear coupling driving term
title_sort practical method for measurement and compensation of linear coupling driving term
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2009-02-01
description We demonstrated a method with practical value for the measurement and global compensation of a complex coupling driving term C of linear difference resonance, using a turn-by-turn beam position monitor (BPM) at the SPring-8 storage ring. The method is based on the perturbation theory with the single-resonance approximation. The accurate complex C was obtained from coefficients of the eigenmode expansion of the coupled betatron oscillation observed near a target linear difference resonance. The global compensation for the measured C was successfully carried out by determining optimal strengths of the two independent correcting skew quadrupoles for generating a counterterm -C without using empirical methods. Meanwhile, we then confirmed that the determined optimal strengths gave a minimum vertical beam size by scanning the strength of the correcting skew quadrupole field. To demonstrate the validity of our method, C was also measured while varying the strengths of the correcting magnets around the optimal values to generate deliberate skew quadrupole error fields. We confirmed that the measured values of C agreed with those coming from the deliberate error fields.
url http://doi.org/10.1103/PhysRevSTAB.12.024002
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