Stripping mechanisms and remediation for H^{-} beams

Negative hydrogen ions are often used for injecting protons from linacs to storage rings via charge-exchange injection. In this process, the two electrons are stripped by a foil or laser to produce protons which can be merged with an existing beam without significantly affecting its dynamics, allowi...

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Main Authors: B. T. Folsom, M. Eshraqi, N. Blaskovic Kraljevic, B. Gålnander
Format: Article
Language:English
Published: American Physical Society 2021-07-01
Series:Physical Review Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevAccelBeams.24.074201
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spelling doaj-1257f25c28224b7f86a31eabdea5b2062021-07-29T18:15:12ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882021-07-0124707420110.1103/PhysRevAccelBeams.24.074201Stripping mechanisms and remediation for H^{-} beamsB. T. FolsomM. EshraqiN. Blaskovic KraljevicB. GålnanderNegative hydrogen ions are often used for injecting protons from linacs to storage rings via charge-exchange injection. In this process, the two electrons are stripped by a foil or laser to produce protons which can be merged with an existing beam without significantly affecting its dynamics, allowing high intensities of protons to be accumulated. However, this capability comes with the drawback that the outer electron of an H^{-} ion has a low binding energy and can easily be stripped away prior to injection. This paper addresses the following stripping mechanisms: interactions with residual gas in the beam pipe, blackbody radiation from accelerator components, and electromagnetic fields from accelerator optics (Lorentz-force stripping) and particles within the bunch itself (intrabeam stripping); with a discussion on how to avoid excessive activation from stripped H^{0} particles and protons. We also demonstrate that the proportion of stripped H^{0} colliding with a nearby beam pipe or machine-element walls presents only roughly 10% of those lost in stripping; the remaining stripped particles traverse to the end of a linac or local straight section, which may relax the limits for allowable stripping-based beam loss in H^{-} accelerators.http://doi.org/10.1103/PhysRevAccelBeams.24.074201
collection DOAJ
language English
format Article
sources DOAJ
author B. T. Folsom
M. Eshraqi
N. Blaskovic Kraljevic
B. Gålnander
spellingShingle B. T. Folsom
M. Eshraqi
N. Blaskovic Kraljevic
B. Gålnander
Stripping mechanisms and remediation for H^{-} beams
Physical Review Accelerators and Beams
author_facet B. T. Folsom
M. Eshraqi
N. Blaskovic Kraljevic
B. Gålnander
author_sort B. T. Folsom
title Stripping mechanisms and remediation for H^{-} beams
title_short Stripping mechanisms and remediation for H^{-} beams
title_full Stripping mechanisms and remediation for H^{-} beams
title_fullStr Stripping mechanisms and remediation for H^{-} beams
title_full_unstemmed Stripping mechanisms and remediation for H^{-} beams
title_sort stripping mechanisms and remediation for h^{-} beams
publisher American Physical Society
series Physical Review Accelerators and Beams
issn 2469-9888
publishDate 2021-07-01
description Negative hydrogen ions are often used for injecting protons from linacs to storage rings via charge-exchange injection. In this process, the two electrons are stripped by a foil or laser to produce protons which can be merged with an existing beam without significantly affecting its dynamics, allowing high intensities of protons to be accumulated. However, this capability comes with the drawback that the outer electron of an H^{-} ion has a low binding energy and can easily be stripped away prior to injection. This paper addresses the following stripping mechanisms: interactions with residual gas in the beam pipe, blackbody radiation from accelerator components, and electromagnetic fields from accelerator optics (Lorentz-force stripping) and particles within the bunch itself (intrabeam stripping); with a discussion on how to avoid excessive activation from stripped H^{0} particles and protons. We also demonstrate that the proportion of stripped H^{0} colliding with a nearby beam pipe or machine-element walls presents only roughly 10% of those lost in stripping; the remaining stripped particles traverse to the end of a linac or local straight section, which may relax the limits for allowable stripping-based beam loss in H^{-} accelerators.
url http://doi.org/10.1103/PhysRevAccelBeams.24.074201
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