Transverse mode-coupling instability and space charge

Transverse mode-coupling instability (TMCI) is known to limit bunch intensity. Since space charge (SC) changes coherent spectra, it affects the TMCI threshold. Generally, there are only two types of TMCI with respect to SC: the vanishing type and the strong space charge (SSC) type. For the former, t...

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Main Authors: T. Zolkin, A. Burov, B. Pandey
Format: Article
Language:English
Published: American Physical Society 2018-10-01
Series:Physical Review Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevAccelBeams.21.104201
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spelling doaj-4d5d80803ffc4bb5b9cf395f922bd1c82020-11-24T22:31:23ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882018-10-01211010420110.1103/PhysRevAccelBeams.21.104201Transverse mode-coupling instability and space chargeT. ZolkinA. BurovB. PandeyTransverse mode-coupling instability (TMCI) is known to limit bunch intensity. Since space charge (SC) changes coherent spectra, it affects the TMCI threshold. Generally, there are only two types of TMCI with respect to SC: the vanishing type and the strong space charge (SSC) type. For the former, the threshold value of the wake tune shift is asymptotically proportional to the SC tune shift, as it was first observed twenty years ago by M. Blaskiewicz for exponential wakes. For the latter, the threshold value of the wake tune shift is asymptotically inversely proportional to the SC, as it was shown by one of the authors. In the presented studies of various wakes, potential wells, and bunch distributions, the second type of instability was always observed for cosine wakes; it was also seen for the sine wakes in the case of a bunch within a square potential well. The vanishing TMCI was observed for all other wakes and distributions we discuss in this paper: always for the negative wakes, and always, except the cosine wake, for parabolic potential wells. At the end of this paper, we consider high-frequency broadband wake, suggested as a model impedance for CERN SPS ring. As expected, TMCI is of the vanishing type in this case. Thus, SPS Q26 instability, observed at strong SC almost with the same bunch parameters as it would be observed without SC, cannot be TMCI.http://doi.org/10.1103/PhysRevAccelBeams.21.104201
collection DOAJ
language English
format Article
sources DOAJ
author T. Zolkin
A. Burov
B. Pandey
spellingShingle T. Zolkin
A. Burov
B. Pandey
Transverse mode-coupling instability and space charge
Physical Review Accelerators and Beams
author_facet T. Zolkin
A. Burov
B. Pandey
author_sort T. Zolkin
title Transverse mode-coupling instability and space charge
title_short Transverse mode-coupling instability and space charge
title_full Transverse mode-coupling instability and space charge
title_fullStr Transverse mode-coupling instability and space charge
title_full_unstemmed Transverse mode-coupling instability and space charge
title_sort transverse mode-coupling instability and space charge
publisher American Physical Society
series Physical Review Accelerators and Beams
issn 2469-9888
publishDate 2018-10-01
description Transverse mode-coupling instability (TMCI) is known to limit bunch intensity. Since space charge (SC) changes coherent spectra, it affects the TMCI threshold. Generally, there are only two types of TMCI with respect to SC: the vanishing type and the strong space charge (SSC) type. For the former, the threshold value of the wake tune shift is asymptotically proportional to the SC tune shift, as it was first observed twenty years ago by M. Blaskiewicz for exponential wakes. For the latter, the threshold value of the wake tune shift is asymptotically inversely proportional to the SC, as it was shown by one of the authors. In the presented studies of various wakes, potential wells, and bunch distributions, the second type of instability was always observed for cosine wakes; it was also seen for the sine wakes in the case of a bunch within a square potential well. The vanishing TMCI was observed for all other wakes and distributions we discuss in this paper: always for the negative wakes, and always, except the cosine wake, for parabolic potential wells. At the end of this paper, we consider high-frequency broadband wake, suggested as a model impedance for CERN SPS ring. As expected, TMCI is of the vanishing type in this case. Thus, SPS Q26 instability, observed at strong SC almost with the same bunch parameters as it would be observed without SC, cannot be TMCI.
url http://doi.org/10.1103/PhysRevAccelBeams.21.104201
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AT aburov transversemodecouplinginstabilityandspacecharge
AT bpandey transversemodecouplinginstabilityandspacecharge
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