Radiation protection designs of the linac for the HEPS
Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam l...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Liu, Qiongyao [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2021 |
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| Schlagwörter: |
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| Anmerkung: |
© Institute of High Energy Physics, Chinese Academy of Sciences 2021 |
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| Übergeordnetes Werk: |
Enthalten in: Radiation detection technology and methods - [Singapore] : Springer Singapore, 2017, 5(2021), 4 vom: 05. Okt., Seite 576-585 |
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| Übergeordnetes Werk: |
volume:5 ; year:2021 ; number:4 ; day:05 ; month:10 ; pages:576-585 |
| Links: |
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| DOI / URN: |
10.1007/s41605-021-00284-3 |
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| Katalog-ID: |
SPR045839077 |
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| 245 | 1 | 0 | |a Radiation protection designs of the linac for the HEPS |
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| 520 | |a Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam loss scenario, optimized thickness for the bulk shielding and detailed structure design for dumps should be proposed. In this paper, the beam loss scenarios were determined and categorized as normal; the dose limits were presented; using these scenarios and the dose limits, the thickness of the linac tunnel was calculated and detailed designs of the main beam dumps were established. The material selection and size setting of the low-power electron beam dump were discussed. Method The Monte Carlo code is a good choice to simulate the radiation analysis. And the iSHIELD11 was used to verify the simulation calculations. Result and conclusion The designs of the linac bulk shield and dumps satisfied the requirements of radiation protection. | ||
| 650 | 4 | |a HEPS |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Linac |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Radiation shielding design |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Dump |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a FLUKA |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a iSHIELD11 |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Ma, Zhongjian |4 aut | |
| 700 | 1 | |a Wu, Qingbiao |4 aut | |
| 700 | 1 | |a Shi, Haoyu |4 aut | |
| 700 | 1 | |a Zhang, Gang |4 aut | |
| 700 | 1 | |a Zhang, Huijie |4 aut | |
| 700 | 1 | |a Liu, Pingcheng |4 aut | |
| 700 | 1 | |a Wang, Qingbin |4 aut | |
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10.1007/s41605-021-00284-3 doi (DE-627)SPR045839077 (SPR)s41605-021-00284-3-e DE-627 ger DE-627 rakwb eng Liu, Qiongyao verfasserin aut Radiation protection designs of the linac for the HEPS 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Institute of High Energy Physics, Chinese Academy of Sciences 2021 Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam loss scenario, optimized thickness for the bulk shielding and detailed structure design for dumps should be proposed. In this paper, the beam loss scenarios were determined and categorized as normal; the dose limits were presented; using these scenarios and the dose limits, the thickness of the linac tunnel was calculated and detailed designs of the main beam dumps were established. The material selection and size setting of the low-power electron beam dump were discussed. Method The Monte Carlo code is a good choice to simulate the radiation analysis. And the iSHIELD11 was used to verify the simulation calculations. Result and conclusion The designs of the linac bulk shield and dumps satisfied the requirements of radiation protection. HEPS (dpeaa)DE-He213 Linac (dpeaa)DE-He213 Radiation shielding design (dpeaa)DE-He213 Dump (dpeaa)DE-He213 FLUKA (dpeaa)DE-He213 iSHIELD11 (dpeaa)DE-He213 Ma, Zhongjian aut Wu, Qingbiao aut Shi, Haoyu aut Zhang, Gang aut Zhang, Huijie aut Liu, Pingcheng aut Wang, Qingbin aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 5(2021), 4 vom: 05. Okt., Seite 576-585 (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:5 year:2021 number:4 day:05 month:10 pages:576-585 https://dx.doi.org/10.1007/s41605-021-00284-3 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 5 2021 4 05 10 576-585 |
| spelling |
10.1007/s41605-021-00284-3 doi (DE-627)SPR045839077 (SPR)s41605-021-00284-3-e DE-627 ger DE-627 rakwb eng Liu, Qiongyao verfasserin aut Radiation protection designs of the linac for the HEPS 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Institute of High Energy Physics, Chinese Academy of Sciences 2021 Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam loss scenario, optimized thickness for the bulk shielding and detailed structure design for dumps should be proposed. In this paper, the beam loss scenarios were determined and categorized as normal; the dose limits were presented; using these scenarios and the dose limits, the thickness of the linac tunnel was calculated and detailed designs of the main beam dumps were established. The material selection and size setting of the low-power electron beam dump were discussed. Method The Monte Carlo code is a good choice to simulate the radiation analysis. And the iSHIELD11 was used to verify the simulation calculations. Result and conclusion The designs of the linac bulk shield and dumps satisfied the requirements of radiation protection. HEPS (dpeaa)DE-He213 Linac (dpeaa)DE-He213 Radiation shielding design (dpeaa)DE-He213 Dump (dpeaa)DE-He213 FLUKA (dpeaa)DE-He213 iSHIELD11 (dpeaa)DE-He213 Ma, Zhongjian aut Wu, Qingbiao aut Shi, Haoyu aut Zhang, Gang aut Zhang, Huijie aut Liu, Pingcheng aut Wang, Qingbin aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 5(2021), 4 vom: 05. Okt., Seite 576-585 (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:5 year:2021 number:4 day:05 month:10 pages:576-585 https://dx.doi.org/10.1007/s41605-021-00284-3 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 5 2021 4 05 10 576-585 |
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10.1007/s41605-021-00284-3 doi (DE-627)SPR045839077 (SPR)s41605-021-00284-3-e DE-627 ger DE-627 rakwb eng Liu, Qiongyao verfasserin aut Radiation protection designs of the linac for the HEPS 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Institute of High Energy Physics, Chinese Academy of Sciences 2021 Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam loss scenario, optimized thickness for the bulk shielding and detailed structure design for dumps should be proposed. In this paper, the beam loss scenarios were determined and categorized as normal; the dose limits were presented; using these scenarios and the dose limits, the thickness of the linac tunnel was calculated and detailed designs of the main beam dumps were established. The material selection and size setting of the low-power electron beam dump were discussed. Method The Monte Carlo code is a good choice to simulate the radiation analysis. And the iSHIELD11 was used to verify the simulation calculations. Result and conclusion The designs of the linac bulk shield and dumps satisfied the requirements of radiation protection. HEPS (dpeaa)DE-He213 Linac (dpeaa)DE-He213 Radiation shielding design (dpeaa)DE-He213 Dump (dpeaa)DE-He213 FLUKA (dpeaa)DE-He213 iSHIELD11 (dpeaa)DE-He213 Ma, Zhongjian aut Wu, Qingbiao aut Shi, Haoyu aut Zhang, Gang aut Zhang, Huijie aut Liu, Pingcheng aut Wang, Qingbin aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 5(2021), 4 vom: 05. Okt., Seite 576-585 (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:5 year:2021 number:4 day:05 month:10 pages:576-585 https://dx.doi.org/10.1007/s41605-021-00284-3 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 5 2021 4 05 10 576-585 |
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10.1007/s41605-021-00284-3 doi (DE-627)SPR045839077 (SPR)s41605-021-00284-3-e DE-627 ger DE-627 rakwb eng Liu, Qiongyao verfasserin aut Radiation protection designs of the linac for the HEPS 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Institute of High Energy Physics, Chinese Academy of Sciences 2021 Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam loss scenario, optimized thickness for the bulk shielding and detailed structure design for dumps should be proposed. In this paper, the beam loss scenarios were determined and categorized as normal; the dose limits were presented; using these scenarios and the dose limits, the thickness of the linac tunnel was calculated and detailed designs of the main beam dumps were established. The material selection and size setting of the low-power electron beam dump were discussed. Method The Monte Carlo code is a good choice to simulate the radiation analysis. And the iSHIELD11 was used to verify the simulation calculations. Result and conclusion The designs of the linac bulk shield and dumps satisfied the requirements of radiation protection. HEPS (dpeaa)DE-He213 Linac (dpeaa)DE-He213 Radiation shielding design (dpeaa)DE-He213 Dump (dpeaa)DE-He213 FLUKA (dpeaa)DE-He213 iSHIELD11 (dpeaa)DE-He213 Ma, Zhongjian aut Wu, Qingbiao aut Shi, Haoyu aut Zhang, Gang aut Zhang, Huijie aut Liu, Pingcheng aut Wang, Qingbin aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 5(2021), 4 vom: 05. Okt., Seite 576-585 (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:5 year:2021 number:4 day:05 month:10 pages:576-585 https://dx.doi.org/10.1007/s41605-021-00284-3 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 5 2021 4 05 10 576-585 |
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10.1007/s41605-021-00284-3 doi (DE-627)SPR045839077 (SPR)s41605-021-00284-3-e DE-627 ger DE-627 rakwb eng Liu, Qiongyao verfasserin aut Radiation protection designs of the linac for the HEPS 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Institute of High Energy Physics, Chinese Academy of Sciences 2021 Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam loss scenario, optimized thickness for the bulk shielding and detailed structure design for dumps should be proposed. In this paper, the beam loss scenarios were determined and categorized as normal; the dose limits were presented; using these scenarios and the dose limits, the thickness of the linac tunnel was calculated and detailed designs of the main beam dumps were established. The material selection and size setting of the low-power electron beam dump were discussed. Method The Monte Carlo code is a good choice to simulate the radiation analysis. And the iSHIELD11 was used to verify the simulation calculations. Result and conclusion The designs of the linac bulk shield and dumps satisfied the requirements of radiation protection. HEPS (dpeaa)DE-He213 Linac (dpeaa)DE-He213 Radiation shielding design (dpeaa)DE-He213 Dump (dpeaa)DE-He213 FLUKA (dpeaa)DE-He213 iSHIELD11 (dpeaa)DE-He213 Ma, Zhongjian aut Wu, Qingbiao aut Shi, Haoyu aut Zhang, Gang aut Zhang, Huijie aut Liu, Pingcheng aut Wang, Qingbin aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 5(2021), 4 vom: 05. Okt., Seite 576-585 (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:5 year:2021 number:4 day:05 month:10 pages:576-585 https://dx.doi.org/10.1007/s41605-021-00284-3 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 5 2021 4 05 10 576-585 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR045839077</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230509100341.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">211224s2021 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s41605-021-00284-3</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR045839077</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s41605-021-00284-3-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Liu, Qiongyao</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Radiation protection designs of the linac for the HEPS</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2021</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Institute of High Energy Physics, Chinese Academy of Sciences 2021</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam loss scenario, optimized thickness for the bulk shielding and detailed structure design for dumps should be proposed. In this paper, the beam loss scenarios were determined and categorized as normal; the dose limits were presented; using these scenarios and the dose limits, the thickness of the linac tunnel was calculated and detailed designs of the main beam dumps were established. The material selection and size setting of the low-power electron beam dump were discussed. Method The Monte Carlo code is a good choice to simulate the radiation analysis. And the iSHIELD11 was used to verify the simulation calculations. 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Liu, Qiongyao |
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Liu, Qiongyao misc HEPS misc Linac misc Radiation shielding design misc Dump misc FLUKA misc iSHIELD11 Radiation protection designs of the linac for the HEPS |
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Radiation protection designs of the linac for the HEPS HEPS (dpeaa)DE-He213 Linac (dpeaa)DE-He213 Radiation shielding design (dpeaa)DE-He213 Dump (dpeaa)DE-He213 FLUKA (dpeaa)DE-He213 iSHIELD11 (dpeaa)DE-He213 |
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misc HEPS misc Linac misc Radiation shielding design misc Dump misc FLUKA misc iSHIELD11 |
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Radiation protection designs of the linac for the HEPS |
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Radiation protection designs of the linac for the HEPS |
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Liu, Qiongyao |
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Radiation detection technology and methods |
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Radiation detection technology and methods |
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Liu, Qiongyao Ma, Zhongjian Wu, Qingbiao Shi, Haoyu Zhang, Gang Zhang, Huijie Liu, Pingcheng Wang, Qingbin |
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Elektronische Aufsätze |
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10.1007/s41605-021-00284-3 |
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radiation protection designs of the linac for the heps |
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Radiation protection designs of the linac for the HEPS |
| abstract |
Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam loss scenario, optimized thickness for the bulk shielding and detailed structure design for dumps should be proposed. In this paper, the beam loss scenarios were determined and categorized as normal; the dose limits were presented; using these scenarios and the dose limits, the thickness of the linac tunnel was calculated and detailed designs of the main beam dumps were established. The material selection and size setting of the low-power electron beam dump were discussed. Method The Monte Carlo code is a good choice to simulate the radiation analysis. And the iSHIELD11 was used to verify the simulation calculations. Result and conclusion The designs of the linac bulk shield and dumps satisfied the requirements of radiation protection. © Institute of High Energy Physics, Chinese Academy of Sciences 2021 |
| abstractGer |
Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam loss scenario, optimized thickness for the bulk shielding and detailed structure design for dumps should be proposed. In this paper, the beam loss scenarios were determined and categorized as normal; the dose limits were presented; using these scenarios and the dose limits, the thickness of the linac tunnel was calculated and detailed designs of the main beam dumps were established. The material selection and size setting of the low-power electron beam dump were discussed. Method The Monte Carlo code is a good choice to simulate the radiation analysis. And the iSHIELD11 was used to verify the simulation calculations. Result and conclusion The designs of the linac bulk shield and dumps satisfied the requirements of radiation protection. © Institute of High Energy Physics, Chinese Academy of Sciences 2021 |
| abstract_unstemmed |
Purpose The high-energy photon source (HEPS) is the first fourth-generation light source under construction in China. It is designed to operate at an average current of 200 mA stored beam current with a top-up model at 6 GeV energy. Considering the linac radiation shielding design, a suitable beam loss scenario, optimized thickness for the bulk shielding and detailed structure design for dumps should be proposed. In this paper, the beam loss scenarios were determined and categorized as normal; the dose limits were presented; using these scenarios and the dose limits, the thickness of the linac tunnel was calculated and detailed designs of the main beam dumps were established. The material selection and size setting of the low-power electron beam dump were discussed. Method The Monte Carlo code is a good choice to simulate the radiation analysis. And the iSHIELD11 was used to verify the simulation calculations. Result and conclusion The designs of the linac bulk shield and dumps satisfied the requirements of radiation protection. © Institute of High Energy Physics, Chinese Academy of Sciences 2021 |
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| title_short |
Radiation protection designs of the linac for the HEPS |
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https://dx.doi.org/10.1007/s41605-021-00284-3 |
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true |
| author2 |
Ma, Zhongjian Wu, Qingbiao Shi, Haoyu Zhang, Gang Zhang, Huijie Liu, Pingcheng Wang, Qingbin |
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Ma, Zhongjian Wu, Qingbiao Shi, Haoyu Zhang, Gang Zhang, Huijie Liu, Pingcheng Wang, Qingbin |
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| doi_str |
10.1007/s41605-021-00284-3 |
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2024-07-03T18:37:24.294Z |
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| score |
7.4010687 |