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Transverse broadband impedance reduction techniques in a heavy ion accelerator

The transverse broadband impedances of major components in the BRing (booster ring) of HIAF (High Intensity Heavy-ion Accelerator Facility) are estimated using the analytical formulas or the wakefield solver in the CST Studio Suite. At low frequency, the transverse broadband impedance model of BRing...

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Autores principales: Chen, X Q, Zhu, G Y, Caspers, F, Yang, J C, Wu, J X, Shen, G D, Liu, J, Xia, J W, Zhang, Y, Ruan, S, Wang, G, Yao, L P, Cai, F C, Ren, H, Kong, Q Y, Gao, Y Z
Lenguaje:eng
Publicado: 2020
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevAccelBeams.23.034402
http://cds.cern.ch/record/2713484
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author Chen, X Q
Zhu, G Y
Caspers, F
Yang, J C
Wu, J X
Shen, G D
Liu, J
Xia, J W
Zhang, Y
Ruan, S
Wang, G
Yao, L P
Cai, F C
Ren, H
Kong, Q Y
Gao, Y Z
author_facet Chen, X Q
Zhu, G Y
Caspers, F
Yang, J C
Wu, J X
Shen, G D
Liu, J
Xia, J W
Zhang, Y
Ruan, S
Wang, G
Yao, L P
Cai, F C
Ren, H
Kong, Q Y
Gao, Y Z
author_sort Chen, X Q
collection CERN
description The transverse broadband impedances of major components in the BRing (booster ring) of HIAF (High Intensity Heavy-ion Accelerator Facility) are estimated using the analytical formulas or the wakefield solver in the CST Studio Suite. At low frequency, the transverse broadband impedance model of BRing is Z1H(ω)=-417.14i  kΩ/m(horizontal) and Z1V(ω)=-530.19i kΩ/m(vertical), which are larger than the threshold impedance for the transverse mode-coupling instability. The ceramic rings in the vacuum chamber are the primary source of impedance. With a goal of mitigating the instability by reducing the impedance of ceramic rings, a high conductivity coating is discussed in detail. In addition, a prototype of ceramic rings-loaded thin-wall vacuum chamber is manufactured and the impedance measurements are performed. When ceramic rings are coated by 2  μm-copper, the CST simulation and experiment results show that the transverse broadband impedance of ceramic rings-loaded thin-wall vacuum chamber can be reduced from Z1H(ω)=-291.69i kΩ/m and Z1V(ω)=-352.37i kΩ/m to Z1H(ω)=-46.16i kΩ/m and Z1V(ω)=-64.56i  kΩ/m. Furthermore, in this case the transverse broadband impedance model of BRing is reduced by more than 50% to Z1H(ω)=-171.61i  kΩ/m and Z1V(ω)=-242.38i  kΩ/m.
id oai-inspirehep.net-1785143
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2020
record_format invenio
spelling oai-inspirehep.net-17851432020-04-01T10:00:22Zdoi:10.1103/PhysRevAccelBeams.23.034402http://cds.cern.ch/record/2713484engChen, X QZhu, G YCaspers, FYang, J CWu, J XShen, G DLiu, JXia, J WZhang, YRuan, SWang, GYao, L PCai, F CRen, HKong, Q YGao, Y ZTransverse broadband impedance reduction techniques in a heavy ion acceleratorAccelerators and Storage RingsThe transverse broadband impedances of major components in the BRing (booster ring) of HIAF (High Intensity Heavy-ion Accelerator Facility) are estimated using the analytical formulas or the wakefield solver in the CST Studio Suite. At low frequency, the transverse broadband impedance model of BRing is Z1H(ω)=-417.14i  kΩ/m(horizontal) and Z1V(ω)=-530.19i kΩ/m(vertical), which are larger than the threshold impedance for the transverse mode-coupling instability. The ceramic rings in the vacuum chamber are the primary source of impedance. With a goal of mitigating the instability by reducing the impedance of ceramic rings, a high conductivity coating is discussed in detail. In addition, a prototype of ceramic rings-loaded thin-wall vacuum chamber is manufactured and the impedance measurements are performed. When ceramic rings are coated by 2  μm-copper, the CST simulation and experiment results show that the transverse broadband impedance of ceramic rings-loaded thin-wall vacuum chamber can be reduced from Z1H(ω)=-291.69i kΩ/m and Z1V(ω)=-352.37i kΩ/m to Z1H(ω)=-46.16i kΩ/m and Z1V(ω)=-64.56i  kΩ/m. Furthermore, in this case the transverse broadband impedance model of BRing is reduced by more than 50% to Z1H(ω)=-171.61i  kΩ/m and Z1V(ω)=-242.38i  kΩ/m.oai:inspirehep.net:17851432020
spellingShingle Accelerators and Storage Rings
Chen, X Q
Zhu, G Y
Caspers, F
Yang, J C
Wu, J X
Shen, G D
Liu, J
Xia, J W
Zhang, Y
Ruan, S
Wang, G
Yao, L P
Cai, F C
Ren, H
Kong, Q Y
Gao, Y Z
Transverse broadband impedance reduction techniques in a heavy ion accelerator
title Transverse broadband impedance reduction techniques in a heavy ion accelerator
title_full Transverse broadband impedance reduction techniques in a heavy ion accelerator
title_fullStr Transverse broadband impedance reduction techniques in a heavy ion accelerator
title_full_unstemmed Transverse broadband impedance reduction techniques in a heavy ion accelerator
title_short Transverse broadband impedance reduction techniques in a heavy ion accelerator
title_sort transverse broadband impedance reduction techniques in a heavy ion accelerator
topic Accelerators and Storage Rings
url https://dx.doi.org/10.1103/PhysRevAccelBeams.23.034402
http://cds.cern.ch/record/2713484
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