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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...
Autores principales: | , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2020
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevAccelBeams.23.034402 http://cds.cern.ch/record/2713484 |
_version_ | 1780965402316111872 |
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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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