Design of proton beam collimation system for HIAF-BRing
Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the unco...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Zheng, Wen-Heng [verfasserIn] |
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E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2022 |
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© The Author(s), under exclusive licence to Institute of High Energy Physics, Chinese Academy of Sciences 2022. Springer Nature or its licensor holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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| Übergeordnetes Werk: |
Enthalten in: Radiation detection technology and methods - [Singapore] : Springer Singapore, 2017, 6(2022), 4 vom: 21. Sept., Seite 519-529 |
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| Übergeordnetes Werk: |
volume:6 ; year:2022 ; number:4 ; day:21 ; month:09 ; pages:519-529 |
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| DOI / URN: |
10.1007/s41605-022-00351-3 |
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| Katalog-ID: |
SPR048532789 |
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| 520 | |a Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the uncontrolled proton beam halo loss around the ring in operation, a two-stage collimation system is proposed to provide a well-shielded dump for localizing the proton beam halo loss. Results and conclusion In this paper, the simulation is carried out to evaluate the collimation system which shows a 92.93% collimation efficiency. Finally, several factors that affect the collimation efficiency are taken into consideration, including the physical aperture, the offset and rotation errors of the collimators, the closed orbit distortion, as well as the Betatron tunes. | ||
| 650 | 4 | |a Proton beam |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Two-stage collimation system |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a ORBIT |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Collimation efficiency |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Yang, Jian-Cheng |4 aut | |
| 700 | 1 | |a Li, Peng |4 aut | |
| 700 | 1 | |a Yin, Da-Yu |4 aut | |
| 700 | 1 | |a Shen, Guo-Dong |4 aut | |
| 700 | 1 | |a Li, Jie |4 aut | |
| 700 | 1 | |a Yao, Li-Ping |4 aut | |
| 700 | 1 | |a Shi, Fu-Dong |4 aut | |
| 700 | 1 | |a Chai, Wei-Ping |4 aut | |
| 700 | 1 | |a Mao, Li-Jun |4 aut | |
| 700 | 1 | |a Li, Wu-yuan |4 aut | |
| 700 | 1 | |a Wang, Geng |4 aut | |
| 700 | 1 | |a Yang, Bo |4 aut | |
| 700 | 1 | |a Luo, Cheng |4 aut | |
| 700 | 1 | |a Ge, Wen-Wen |4 aut | |
| 700 | 1 | |a Li, Zhong-Shan |4 aut | |
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10.1007/s41605-022-00351-3 doi (DE-627)SPR048532789 (SPR)s41605-022-00351-3-e DE-627 ger DE-627 rakwb eng Zheng, Wen-Heng verfasserin (orcid)0000-0002-9658-7138 aut Design of proton beam collimation system for HIAF-BRing 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Institute of High Energy Physics, Chinese Academy of Sciences 2022. Springer Nature or its licensor holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the uncontrolled proton beam halo loss around the ring in operation, a two-stage collimation system is proposed to provide a well-shielded dump for localizing the proton beam halo loss. Results and conclusion In this paper, the simulation is carried out to evaluate the collimation system which shows a 92.93% collimation efficiency. Finally, several factors that affect the collimation efficiency are taken into consideration, including the physical aperture, the offset and rotation errors of the collimators, the closed orbit distortion, as well as the Betatron tunes. Proton beam (dpeaa)DE-He213 Two-stage collimation system (dpeaa)DE-He213 ORBIT (dpeaa)DE-He213 Collimation efficiency (dpeaa)DE-He213 Yang, Jian-Cheng aut Li, Peng aut Yin, Da-Yu aut Shen, Guo-Dong aut Li, Jie aut Yao, Li-Ping aut Shi, Fu-Dong aut Chai, Wei-Ping aut Mao, Li-Jun aut Li, Wu-yuan aut Wang, Geng aut Yang, Bo aut Luo, Cheng aut Ge, Wen-Wen aut Li, Zhong-Shan aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 6(2022), 4 vom: 21. Sept., Seite 519-529 (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:6 year:2022 number:4 day:21 month:09 pages:519-529 https://dx.doi.org/10.1007/s41605-022-00351-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 6 2022 4 21 09 519-529 |
| spelling |
10.1007/s41605-022-00351-3 doi (DE-627)SPR048532789 (SPR)s41605-022-00351-3-e DE-627 ger DE-627 rakwb eng Zheng, Wen-Heng verfasserin (orcid)0000-0002-9658-7138 aut Design of proton beam collimation system for HIAF-BRing 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Institute of High Energy Physics, Chinese Academy of Sciences 2022. Springer Nature or its licensor holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the uncontrolled proton beam halo loss around the ring in operation, a two-stage collimation system is proposed to provide a well-shielded dump for localizing the proton beam halo loss. Results and conclusion In this paper, the simulation is carried out to evaluate the collimation system which shows a 92.93% collimation efficiency. Finally, several factors that affect the collimation efficiency are taken into consideration, including the physical aperture, the offset and rotation errors of the collimators, the closed orbit distortion, as well as the Betatron tunes. Proton beam (dpeaa)DE-He213 Two-stage collimation system (dpeaa)DE-He213 ORBIT (dpeaa)DE-He213 Collimation efficiency (dpeaa)DE-He213 Yang, Jian-Cheng aut Li, Peng aut Yin, Da-Yu aut Shen, Guo-Dong aut Li, Jie aut Yao, Li-Ping aut Shi, Fu-Dong aut Chai, Wei-Ping aut Mao, Li-Jun aut Li, Wu-yuan aut Wang, Geng aut Yang, Bo aut Luo, Cheng aut Ge, Wen-Wen aut Li, Zhong-Shan aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 6(2022), 4 vom: 21. Sept., Seite 519-529 (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:6 year:2022 number:4 day:21 month:09 pages:519-529 https://dx.doi.org/10.1007/s41605-022-00351-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 6 2022 4 21 09 519-529 |
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10.1007/s41605-022-00351-3 doi (DE-627)SPR048532789 (SPR)s41605-022-00351-3-e DE-627 ger DE-627 rakwb eng Zheng, Wen-Heng verfasserin (orcid)0000-0002-9658-7138 aut Design of proton beam collimation system for HIAF-BRing 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Institute of High Energy Physics, Chinese Academy of Sciences 2022. Springer Nature or its licensor holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the uncontrolled proton beam halo loss around the ring in operation, a two-stage collimation system is proposed to provide a well-shielded dump for localizing the proton beam halo loss. Results and conclusion In this paper, the simulation is carried out to evaluate the collimation system which shows a 92.93% collimation efficiency. Finally, several factors that affect the collimation efficiency are taken into consideration, including the physical aperture, the offset and rotation errors of the collimators, the closed orbit distortion, as well as the Betatron tunes. Proton beam (dpeaa)DE-He213 Two-stage collimation system (dpeaa)DE-He213 ORBIT (dpeaa)DE-He213 Collimation efficiency (dpeaa)DE-He213 Yang, Jian-Cheng aut Li, Peng aut Yin, Da-Yu aut Shen, Guo-Dong aut Li, Jie aut Yao, Li-Ping aut Shi, Fu-Dong aut Chai, Wei-Ping aut Mao, Li-Jun aut Li, Wu-yuan aut Wang, Geng aut Yang, Bo aut Luo, Cheng aut Ge, Wen-Wen aut Li, Zhong-Shan aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 6(2022), 4 vom: 21. Sept., Seite 519-529 (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:6 year:2022 number:4 day:21 month:09 pages:519-529 https://dx.doi.org/10.1007/s41605-022-00351-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 6 2022 4 21 09 519-529 |
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10.1007/s41605-022-00351-3 doi (DE-627)SPR048532789 (SPR)s41605-022-00351-3-e DE-627 ger DE-627 rakwb eng Zheng, Wen-Heng verfasserin (orcid)0000-0002-9658-7138 aut Design of proton beam collimation system for HIAF-BRing 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Institute of High Energy Physics, Chinese Academy of Sciences 2022. Springer Nature or its licensor holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the uncontrolled proton beam halo loss around the ring in operation, a two-stage collimation system is proposed to provide a well-shielded dump for localizing the proton beam halo loss. Results and conclusion In this paper, the simulation is carried out to evaluate the collimation system which shows a 92.93% collimation efficiency. Finally, several factors that affect the collimation efficiency are taken into consideration, including the physical aperture, the offset and rotation errors of the collimators, the closed orbit distortion, as well as the Betatron tunes. Proton beam (dpeaa)DE-He213 Two-stage collimation system (dpeaa)DE-He213 ORBIT (dpeaa)DE-He213 Collimation efficiency (dpeaa)DE-He213 Yang, Jian-Cheng aut Li, Peng aut Yin, Da-Yu aut Shen, Guo-Dong aut Li, Jie aut Yao, Li-Ping aut Shi, Fu-Dong aut Chai, Wei-Ping aut Mao, Li-Jun aut Li, Wu-yuan aut Wang, Geng aut Yang, Bo aut Luo, Cheng aut Ge, Wen-Wen aut Li, Zhong-Shan aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 6(2022), 4 vom: 21. Sept., Seite 519-529 (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:6 year:2022 number:4 day:21 month:09 pages:519-529 https://dx.doi.org/10.1007/s41605-022-00351-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 6 2022 4 21 09 519-529 |
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10.1007/s41605-022-00351-3 doi (DE-627)SPR048532789 (SPR)s41605-022-00351-3-e DE-627 ger DE-627 rakwb eng Zheng, Wen-Heng verfasserin (orcid)0000-0002-9658-7138 aut Design of proton beam collimation system for HIAF-BRing 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Institute of High Energy Physics, Chinese Academy of Sciences 2022. Springer Nature or its licensor holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the uncontrolled proton beam halo loss around the ring in operation, a two-stage collimation system is proposed to provide a well-shielded dump for localizing the proton beam halo loss. Results and conclusion In this paper, the simulation is carried out to evaluate the collimation system which shows a 92.93% collimation efficiency. Finally, several factors that affect the collimation efficiency are taken into consideration, including the physical aperture, the offset and rotation errors of the collimators, the closed orbit distortion, as well as the Betatron tunes. Proton beam (dpeaa)DE-He213 Two-stage collimation system (dpeaa)DE-He213 ORBIT (dpeaa)DE-He213 Collimation efficiency (dpeaa)DE-He213 Yang, Jian-Cheng aut Li, Peng aut Yin, Da-Yu aut Shen, Guo-Dong aut Li, Jie aut Yao, Li-Ping aut Shi, Fu-Dong aut Chai, Wei-Ping aut Mao, Li-Jun aut Li, Wu-yuan aut Wang, Geng aut Yang, Bo aut Luo, Cheng aut Ge, Wen-Wen aut Li, Zhong-Shan aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 6(2022), 4 vom: 21. Sept., Seite 519-529 (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:6 year:2022 number:4 day:21 month:09 pages:519-529 https://dx.doi.org/10.1007/s41605-022-00351-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 6 2022 4 21 09 519-529 |
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Springer Nature or its licensor holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the uncontrolled proton beam halo loss around the ring in operation, a two-stage collimation system is proposed to provide a well-shielded dump for localizing the proton beam halo loss. Results and conclusion In this paper, the simulation is carried out to evaluate the collimation system which shows a 92.93% collimation efficiency. 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Design of proton beam collimation system for HIAF-BRing Proton beam (dpeaa)DE-He213 Two-stage collimation system (dpeaa)DE-He213 ORBIT (dpeaa)DE-He213 Collimation efficiency (dpeaa)DE-He213 |
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Zheng, Wen-Heng Yang, Jian-Cheng Li, Peng Yin, Da-Yu Shen, Guo-Dong Li, Jie Yao, Li-Ping Shi, Fu-Dong Chai, Wei-Ping Mao, Li-Jun Li, Wu-yuan Wang, Geng Yang, Bo Luo, Cheng Ge, Wen-Wen Li, Zhong-Shan |
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design of proton beam collimation system for hiaf-bring |
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Design of proton beam collimation system for HIAF-BRing |
| abstract |
Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the uncontrolled proton beam halo loss around the ring in operation, a two-stage collimation system is proposed to provide a well-shielded dump for localizing the proton beam halo loss. Results and conclusion In this paper, the simulation is carried out to evaluate the collimation system which shows a 92.93% collimation efficiency. Finally, several factors that affect the collimation efficiency are taken into consideration, including the physical aperture, the offset and rotation errors of the collimators, the closed orbit distortion, as well as the Betatron tunes. © The Author(s), under exclusive licence to Institute of High Energy Physics, Chinese Academy of Sciences 2022. Springer Nature or its licensor holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstractGer |
Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the uncontrolled proton beam halo loss around the ring in operation, a two-stage collimation system is proposed to provide a well-shielded dump for localizing the proton beam halo loss. Results and conclusion In this paper, the simulation is carried out to evaluate the collimation system which shows a 92.93% collimation efficiency. Finally, several factors that affect the collimation efficiency are taken into consideration, including the physical aperture, the offset and rotation errors of the collimators, the closed orbit distortion, as well as the Betatron tunes. © The Author(s), under exclusive licence to Institute of High Energy Physics, Chinese Academy of Sciences 2022. Springer Nature or its licensor holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstract_unstemmed |
Background The Booster Ring is further designed to store and accelerate protons up to 2 × $ 10^{12} $ particles per pulse in the High-Intensity heavy-ion Accelerator Facility project, which was originally designed to accelerate high-intensity heavy ion beams. Purpose and Methods To minimize the uncontrolled proton beam halo loss around the ring in operation, a two-stage collimation system is proposed to provide a well-shielded dump for localizing the proton beam halo loss. Results and conclusion In this paper, the simulation is carried out to evaluate the collimation system which shows a 92.93% collimation efficiency. Finally, several factors that affect the collimation efficiency are taken into consideration, including the physical aperture, the offset and rotation errors of the collimators, the closed orbit distortion, as well as the Betatron tunes. © The Author(s), under exclusive licence to Institute of High Energy Physics, Chinese Academy of Sciences 2022. Springer Nature or its licensor holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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Design of proton beam collimation system for HIAF-BRing |
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https://dx.doi.org/10.1007/s41605-022-00351-3 |
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Yang, Jian-Cheng Li, Peng Yin, Da-Yu Shen, Guo-Dong Li, Jie Yao, Li-Ping Shi, Fu-Dong Chai, Wei-Ping Mao, Li-Jun Li, Wu-yuan Wang, Geng Yang, Bo Luo, Cheng Ge, Wen-Wen Li, Zhong-Shan |
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Yang, Jian-Cheng Li, Peng Yin, Da-Yu Shen, Guo-Dong Li, Jie Yao, Li-Ping Shi, Fu-Dong Chai, Wei-Ping Mao, Li-Jun Li, Wu-yuan Wang, Geng Yang, Bo Luo, Cheng Ge, Wen-Wen Li, Zhong-Shan |
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10.1007/s41605-022-00351-3 |
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2024-07-03T19:50:07.694Z |
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| score |
7.4014387 |