Tune shifts of bunch trains due to resistive vacuum chambers without circular symmetry

We present an explanation for the opposite signs of the horizontal and vertical tune shifts of bunch trains which have been observed recently in several high-energy storage rings. This result can be understood in terms of the long-range quadrupolar wakes of noncircular vacuum chambers with finite re...

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Main Authors: Alexander Chao, Samuel Heifets, Bruno Zotter
Format: Article
Language:English
Published: American Physical Society 2002-11-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.5.111001
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spelling doaj-aa3461eb125a44bcb2f238e7e646799d2020-11-25T02:19:07ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022002-11-0151111100110.1103/PhysRevSTAB.5.111001Tune shifts of bunch trains due to resistive vacuum chambers without circular symmetryAlexander ChaoSamuel HeifetsBruno ZotterWe present an explanation for the opposite signs of the horizontal and vertical tune shifts of bunch trains which have been observed recently in several high-energy storage rings. This result can be understood in terms of the long-range quadrupolar wakes of noncircular vacuum chambers with finite resistivity. In vacuum chambers with circular cross section, the dominant transverse wake driven by a leading particle and seen by a trailing test particle is dipolar and is proportional only to the transverse offset of the driving particle. The contributions of preceding bunches or previous turns tend to cancel, as they add with oscillatory factors. On the other hand, quadrupolar wakes are independent of the offset of the driving particle, and thus the contributions of preceding bunches and turns are strictly additive. Since quadrupole fields are focusing in one plane and defocusing in the plane orthogonal to it, their effects on tune shifts in these planes have opposite signs. Their cumulative effect also explains the large values of the tune shifts measured in PEP-II, which exceeded estimates from other impedance sources by factors of 3 to 4. Our analysis also offers a connection to the familiar Laslett tune shift.http://doi.org/10.1103/PhysRevSTAB.5.111001
collection DOAJ
language English
format Article
sources DOAJ
author Alexander Chao
Samuel Heifets
Bruno Zotter
spellingShingle Alexander Chao
Samuel Heifets
Bruno Zotter
Tune shifts of bunch trains due to resistive vacuum chambers without circular symmetry
Physical Review Special Topics. Accelerators and Beams
author_facet Alexander Chao
Samuel Heifets
Bruno Zotter
author_sort Alexander Chao
title Tune shifts of bunch trains due to resistive vacuum chambers without circular symmetry
title_short Tune shifts of bunch trains due to resistive vacuum chambers without circular symmetry
title_full Tune shifts of bunch trains due to resistive vacuum chambers without circular symmetry
title_fullStr Tune shifts of bunch trains due to resistive vacuum chambers without circular symmetry
title_full_unstemmed Tune shifts of bunch trains due to resistive vacuum chambers without circular symmetry
title_sort tune shifts of bunch trains due to resistive vacuum chambers without circular symmetry
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2002-11-01
description We present an explanation for the opposite signs of the horizontal and vertical tune shifts of bunch trains which have been observed recently in several high-energy storage rings. This result can be understood in terms of the long-range quadrupolar wakes of noncircular vacuum chambers with finite resistivity. In vacuum chambers with circular cross section, the dominant transverse wake driven by a leading particle and seen by a trailing test particle is dipolar and is proportional only to the transverse offset of the driving particle. The contributions of preceding bunches or previous turns tend to cancel, as they add with oscillatory factors. On the other hand, quadrupolar wakes are independent of the offset of the driving particle, and thus the contributions of preceding bunches and turns are strictly additive. Since quadrupole fields are focusing in one plane and defocusing in the plane orthogonal to it, their effects on tune shifts in these planes have opposite signs. Their cumulative effect also explains the large values of the tune shifts measured in PEP-II, which exceeded estimates from other impedance sources by factors of 3 to 4. Our analysis also offers a connection to the familiar Laslett tune shift.
url http://doi.org/10.1103/PhysRevSTAB.5.111001
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