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Recent RHIC in-situ coating technology developments
To rectify the problems of electron clouds observed in RHIC and unacceptable ohmic heating for superconducting magnets that can limit future machine upgrades, we started developing a robotic plasma deposition technique for $in-situ$ coating of the RHIC 316LN stainless steel cold bore tubes based on...
Autores principales: | , , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2013
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.5170/CERN-2013-002.251 http://cds.cern.ch/record/1566377 |
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author | Hershcovitch, A. Blaskiewicz, M. Brennan, J.M. Chawla, A. Fischer, W. Liaw, C-J Meng, W. Todd, R. Custer, A. Erickson, M. Jamshidi, N. Kobrin, P. Laping, R. Poole, H.J. Jimenez, J.M. Neupert, H. Taborelli, M. Yin-Vallgren, C. Sochugov, N. |
author_facet | Hershcovitch, A. Blaskiewicz, M. Brennan, J.M. Chawla, A. Fischer, W. Liaw, C-J Meng, W. Todd, R. Custer, A. Erickson, M. Jamshidi, N. Kobrin, P. Laping, R. Poole, H.J. Jimenez, J.M. Neupert, H. Taborelli, M. Yin-Vallgren, C. Sochugov, N. |
author_sort | Hershcovitch, A. |
collection | CERN |
description | To rectify the problems of electron clouds observed in RHIC and unacceptable ohmic heating for superconducting magnets that can limit future machine upgrades, we started developing a robotic plasma deposition technique for $in-situ$ coating of the RHIC 316LN stainless steel cold bore tubes based on staged magnetrons mounted on a mobile mole for deposition of Cu followed by amorphous carbon (a-C) coating. The Cu coating reduces wall resistivity, while a-C has low SEY that suppresses electron cloud formation. Recent RF resistivity computations indicate that 10 {\mu}m of Cu coating thickness is needed. But, Cu coatings thicker than 2 {\mu}m can have grain structures that might have lower SEY like gold black. A 15-cm Cu cathode magnetron was designed and fabricated, after which, 30 cm long samples of RHIC cold bore tubes were coated with various OFHC copper thicknesses; room temperature RF resistivity measured. Rectangular stainless steel and SS discs were Cu coated. SEY of rectangular samples were measured at room; and, SEY of a disc sample was measured at cryogenic temperatures. |
id | cern-1566377 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2013 |
record_format | invenio |
spelling | cern-15663772022-08-10T20:57:49Zdoi:10.5170/CERN-2013-002.251http://cds.cern.ch/record/1566377engHershcovitch, A.Blaskiewicz, M.Brennan, J.M.Chawla, A.Fischer, W.Liaw, C-JMeng, W.Todd, R.Custer, A.Erickson, M.Jamshidi, N.Kobrin, P.Laping, R.Poole, H.J.Jimenez, J.M.Neupert, H.Taborelli, M.Yin-Vallgren, C.Sochugov, N.Recent RHIC in-situ coating technology developmentsAccelerators and Storage RingsTo rectify the problems of electron clouds observed in RHIC and unacceptable ohmic heating for superconducting magnets that can limit future machine upgrades, we started developing a robotic plasma deposition technique for $in-situ$ coating of the RHIC 316LN stainless steel cold bore tubes based on staged magnetrons mounted on a mobile mole for deposition of Cu followed by amorphous carbon (a-C) coating. The Cu coating reduces wall resistivity, while a-C has low SEY that suppresses electron cloud formation. Recent RF resistivity computations indicate that 10 {\mu}m of Cu coating thickness is needed. But, Cu coatings thicker than 2 {\mu}m can have grain structures that might have lower SEY like gold black. A 15-cm Cu cathode magnetron was designed and fabricated, after which, 30 cm long samples of RHIC cold bore tubes were coated with various OFHC copper thicknesses; room temperature RF resistivity measured. Rectangular stainless steel and SS discs were Cu coated. SEY of rectangular samples were measured at room; and, SEY of a disc sample was measured at cryogenic temperatures.To rectify the problems of electron clouds observed in RHIC and unacceptable ohmic heating for superconducting magnets that can limit future machine upgrades, we started developing a robotic plasma deposition technique for $in-situ$ coating of the RHIC 316LN stainless steel cold bore tubes based on staged magnetrons mounted on a mobile mole for deposition of Cu followed by amorphous carbon (a-C) coating. The Cu coating reduces wall resistivity, while a-C has low SEY that suppresses electron cloud formation. Recent RF resistivity computations indicate that 10 {\mu}m of Cu coating thickness is needed. But, Cu coatings thicker than 2 {\mu}m can have grain structures that might have lower SEY like gold black. A 15-cm Cu cathode magnetron was designed and fabricated, after which, 30 cm long samples of RHIC cold bore tubes were coated with various OFHC copper thicknesses; room temperature RF resistivity measured. Rectangular stainless steel and SS discs were Cu coated. SEY of rectangular samples were measured at room; and, SEY of a disc sample was measured at cryogenic temperatures.arXiv:1308.0125oai:cds.cern.ch:15663772013-08-01 |
spellingShingle | Accelerators and Storage Rings Hershcovitch, A. Blaskiewicz, M. Brennan, J.M. Chawla, A. Fischer, W. Liaw, C-J Meng, W. Todd, R. Custer, A. Erickson, M. Jamshidi, N. Kobrin, P. Laping, R. Poole, H.J. Jimenez, J.M. Neupert, H. Taborelli, M. Yin-Vallgren, C. Sochugov, N. Recent RHIC in-situ coating technology developments |
title | Recent RHIC in-situ coating technology developments |
title_full | Recent RHIC in-situ coating technology developments |
title_fullStr | Recent RHIC in-situ coating technology developments |
title_full_unstemmed | Recent RHIC in-situ coating technology developments |
title_short | Recent RHIC in-situ coating technology developments |
title_sort | recent rhic in-situ coating technology developments |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.5170/CERN-2013-002.251 http://cds.cern.ch/record/1566377 |
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