Fixed field alternating gradient accelerator with small orbit shift and tune excursion

A new design principle of a nonscaling fixed field alternating gradient accelerator is proposed. It is based on optics that produce approximate scaling properties. A large field index k is chosen to squeeze the orbit shift as much as possible by setting the betatron oscillation frequency in the seco...

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Main Authors: Suzanne L. Sheehy, Ken J. Peach, Holger Witte, David J. Kelliher, Shinji Machida
Format: Article
Language:English
Published: American Physical Society 2010-04-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.13.040101
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spelling doaj-000139c08f864737a02755fffb8ef9ee2020-11-24T21:31:44ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022010-04-0113404010110.1103/PhysRevSTAB.13.040101Fixed field alternating gradient accelerator with small orbit shift and tune excursionSuzanne L. SheehyKen J. PeachHolger WitteDavid J. KelliherShinji MachidaA new design principle of a nonscaling fixed field alternating gradient accelerator is proposed. It is based on optics that produce approximate scaling properties. A large field index k is chosen to squeeze the orbit shift as much as possible by setting the betatron oscillation frequency in the second stability region of Hill’s equation. Then, the lattice magnets and their alignment are simplified. To simplify the magnets, we expand the field profile of r^{k} into multipoles and keep only a few lower order terms. A rectangular-shaped magnet is assumed with lines of constant field parallel to the magnet axis. The lattice employs a triplet of rectangular magnets for focusing, which are parallel to one another to simplify alignment. These simplifications along with fringe fields introduce finite chromaticity and the fixed field alternating gradient accelerator is no longer a scaling one. However, the tune excursion of the whole ring can be within half an integer and we avoid the crossing of strong resonances.http://doi.org/10.1103/PhysRevSTAB.13.040101
collection DOAJ
language English
format Article
sources DOAJ
author Suzanne L. Sheehy
Ken J. Peach
Holger Witte
David J. Kelliher
Shinji Machida
spellingShingle Suzanne L. Sheehy
Ken J. Peach
Holger Witte
David J. Kelliher
Shinji Machida
Fixed field alternating gradient accelerator with small orbit shift and tune excursion
Physical Review Special Topics. Accelerators and Beams
author_facet Suzanne L. Sheehy
Ken J. Peach
Holger Witte
David J. Kelliher
Shinji Machida
author_sort Suzanne L. Sheehy
title Fixed field alternating gradient accelerator with small orbit shift and tune excursion
title_short Fixed field alternating gradient accelerator with small orbit shift and tune excursion
title_full Fixed field alternating gradient accelerator with small orbit shift and tune excursion
title_fullStr Fixed field alternating gradient accelerator with small orbit shift and tune excursion
title_full_unstemmed Fixed field alternating gradient accelerator with small orbit shift and tune excursion
title_sort fixed field alternating gradient accelerator with small orbit shift and tune excursion
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2010-04-01
description A new design principle of a nonscaling fixed field alternating gradient accelerator is proposed. It is based on optics that produce approximate scaling properties. A large field index k is chosen to squeeze the orbit shift as much as possible by setting the betatron oscillation frequency in the second stability region of Hill’s equation. Then, the lattice magnets and their alignment are simplified. To simplify the magnets, we expand the field profile of r^{k} into multipoles and keep only a few lower order terms. A rectangular-shaped magnet is assumed with lines of constant field parallel to the magnet axis. The lattice employs a triplet of rectangular magnets for focusing, which are parallel to one another to simplify alignment. These simplifications along with fringe fields introduce finite chromaticity and the fixed field alternating gradient accelerator is no longer a scaling one. However, the tune excursion of the whole ring can be within half an integer and we avoid the crossing of strong resonances.
url http://doi.org/10.1103/PhysRevSTAB.13.040101
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