Polarized ^{3}He^{+2} ions in the Alternate Gradient Synchrotron to RHIC transfer line

The proposed electron-hadron collider (eRHIC) to be built at Brookhaven National Laboratory (BNL) will allow the collisions of 20 GeV polarized electrons with 250 GeV polarized protons, or 100  GeV/n polarized ^{3}He^{+2} ions, or other unpolarized ion species. The large value of the anomalous magne...

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Main Authors: N. Tsoupas, H. Huang, F. Méot, V. Ptitsyn, T. Roser, D. Trbojevic
Format: Article
Language:English
Published: American Physical Society 2016-09-01
Series:Physical Review Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevAccelBeams.19.094702
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spelling doaj-826d897005ca4baa8acbe11ecd0e02c12020-11-24T21:02:18ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882016-09-0119909470210.1103/PhysRevAccelBeams.19.094702Polarized ^{3}He^{+2} ions in the Alternate Gradient Synchrotron to RHIC transfer lineN. TsoupasH. HuangF. MéotV. PtitsynT. RoserD. TrbojevicThe proposed electron-hadron collider (eRHIC) to be built at Brookhaven National Laboratory (BNL) will allow the collisions of 20 GeV polarized electrons with 250 GeV polarized protons, or 100  GeV/n polarized ^{3}He^{+2} ions, or other unpolarized ion species. The large value of the anomalous magnetic moment of the ^{3}He nucleus G_{He}=(g-2)/2=-4.184 (where g is the g-factor of the ^{3}He nuclear spin) combined with the peculiar layout of the transfer line which transports the beam bunches from the Alternate Gradient Synchrotron (AGS) to the Relativistic Heavy Ion Collider (RHIC) makes the transfer and injection of polarized ^{3}He ions from AGS to RHIC (AtR) a special case as we explain in the paper. Specifically in this paper we calculate the stable spin direction of a polarized ^{3}He beam at the exit of the AtR line which is also the injection point of RHIC, and we discuss a simple modifications of the AtR beam-transfer-line, to perfectly match the stable spin direction of the injected polarized ^{3}He beam to that of the circulating beam, at the injection point of RHIC.http://doi.org/10.1103/PhysRevAccelBeams.19.094702
collection DOAJ
language English
format Article
sources DOAJ
author N. Tsoupas
H. Huang
F. Méot
V. Ptitsyn
T. Roser
D. Trbojevic
spellingShingle N. Tsoupas
H. Huang
F. Méot
V. Ptitsyn
T. Roser
D. Trbojevic
Polarized ^{3}He^{+2} ions in the Alternate Gradient Synchrotron to RHIC transfer line
Physical Review Accelerators and Beams
author_facet N. Tsoupas
H. Huang
F. Méot
V. Ptitsyn
T. Roser
D. Trbojevic
author_sort N. Tsoupas
title Polarized ^{3}He^{+2} ions in the Alternate Gradient Synchrotron to RHIC transfer line
title_short Polarized ^{3}He^{+2} ions in the Alternate Gradient Synchrotron to RHIC transfer line
title_full Polarized ^{3}He^{+2} ions in the Alternate Gradient Synchrotron to RHIC transfer line
title_fullStr Polarized ^{3}He^{+2} ions in the Alternate Gradient Synchrotron to RHIC transfer line
title_full_unstemmed Polarized ^{3}He^{+2} ions in the Alternate Gradient Synchrotron to RHIC transfer line
title_sort polarized ^{3}he^{+2} ions in the alternate gradient synchrotron to rhic transfer line
publisher American Physical Society
series Physical Review Accelerators and Beams
issn 2469-9888
publishDate 2016-09-01
description The proposed electron-hadron collider (eRHIC) to be built at Brookhaven National Laboratory (BNL) will allow the collisions of 20 GeV polarized electrons with 250 GeV polarized protons, or 100  GeV/n polarized ^{3}He^{+2} ions, or other unpolarized ion species. The large value of the anomalous magnetic moment of the ^{3}He nucleus G_{He}=(g-2)/2=-4.184 (where g is the g-factor of the ^{3}He nuclear spin) combined with the peculiar layout of the transfer line which transports the beam bunches from the Alternate Gradient Synchrotron (AGS) to the Relativistic Heavy Ion Collider (RHIC) makes the transfer and injection of polarized ^{3}He ions from AGS to RHIC (AtR) a special case as we explain in the paper. Specifically in this paper we calculate the stable spin direction of a polarized ^{3}He beam at the exit of the AtR line which is also the injection point of RHIC, and we discuss a simple modifications of the AtR beam-transfer-line, to perfectly match the stable spin direction of the injected polarized ^{3}He beam to that of the circulating beam, at the injection point of RHIC.
url http://doi.org/10.1103/PhysRevAccelBeams.19.094702
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