The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS
Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitiv...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Ren, Jie [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2019 |
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| Schlagwörter: |
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| Anmerkung: |
© Institute of High Energy Physics, Chinese Academy of Sciences; Nuclear Electronics and Nuclear Detection Society 2019 |
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| Übergeordnetes Werk: |
Enthalten in: Radiation detection technology and methods - [Singapore] : Springer Singapore, 2017, 3(2019), 3 vom: 18. Juni |
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| Übergeordnetes Werk: |
volume:3 ; year:2019 ; number:3 ; day:18 ; month:06 |
| Links: |
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| DOI / URN: |
10.1007/s41605-019-0129-8 |
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| Katalog-ID: |
SPR038252805 |
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|---|---|---|---|
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| 003 | DE-627 | ||
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| 008 | 201007s2019 xx |||||o 00| ||eng c | ||
| 024 | 7 | |a 10.1007/s41605-019-0129-8 |2 doi | |
| 035 | |a (DE-627)SPR038252805 | ||
| 035 | |a (SPR)s41605-019-0129-8-e | ||
| 040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
| 041 | |a eng | ||
| 100 | 1 | |a Ren, Jie |e verfasserin |0 (orcid)0000-0003-2738-537X |4 aut | |
| 245 | 1 | 4 | |a The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS |
| 264 | 1 | |c 2019 | |
| 336 | |a Text |b txt |2 rdacontent | ||
| 337 | |a Computermedien |b c |2 rdamedia | ||
| 338 | |a Online-Ressource |b cr |2 rdacarrier | ||
| 500 | |a © Institute of High Energy Physics, Chinese Academy of Sciences; Nuclear Electronics and Nuclear Detection Society 2019 | ||
| 520 | |a Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitivity and fast time response. The Back-n white neutron source at China Spallation Neutron Source is the first spallation white neutron source in China, and it is suitable for neutron capture cross-sectional measurement. Materials and methods A $ C_{6} %$ D_{6} $ detector system was built in the Back-n experimental station. The pulse height weighting technique was used to determine the system’s detection efficiency. The response to gamma rays of the $ C_{6} %$ D_{6} $ detector was measured, and the energy resolution function was determined. Monte Carlo simulation with Geant4 code was carried out to get the weighting function of this $ C_{6} %$ D_{6} $ detector system. Additionally, the systematic uncertainty of the weighting function was also determined. Conclusion According to the experimental and simulation results, this $ C_{6} %$ D_{6} $ detector system can be used to measure neutron capture cross section. | ||
| 650 | 4 | |a C |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a D |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a detector |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a PHWT |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Neutron capture cross section |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a White neutron source |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Ruan, Xichao |4 aut | |
| 700 | 1 | |a Bao, Jie |4 aut | |
| 700 | 1 | |a Luan, Guangyuan |4 aut | |
| 700 | 1 | |a Jiang, Wei |4 aut | |
| 700 | 1 | |a An, Qi |4 aut | |
| 700 | 1 | |a Bai, Huaiyong |4 aut | |
| 700 | 1 | |a Cao, Ping |4 aut | |
| 700 | 1 | |a Chen, Qiping |4 aut | |
| 700 | 1 | |a Chen, Yonghao |4 aut | |
| 700 | 1 | |a Cheng, Pinjing |4 aut | |
| 700 | 1 | |a Cui, Zengqi |4 aut | |
| 700 | 1 | |a Fan, Ruirui |4 aut | |
| 700 | 1 | |a Feng, Changqing |4 aut | |
| 700 | 1 | |a Gu, Minhao |4 aut | |
| 700 | 1 | |a Guo, Fengqin |4 aut | |
| 700 | 1 | |a Han, Changcai |4 aut | |
| 700 | 1 | |a Han, Zijie |4 aut | |
| 700 | 1 | |a He, Guozhu |4 aut | |
| 700 | 1 | |a He, Yongcheng |4 aut | |
| 700 | 1 | |a He, Yuefeng |4 aut | |
| 700 | 1 | |a Huang, Hanxiong |4 aut | |
| 700 | 1 | |a Huang, Weiling |4 aut | |
| 700 | 1 | |a Huang, Xiru |4 aut | |
| 700 | 1 | |a Ji, Xiaolu |4 aut | |
| 700 | 1 | |a Ji, Xuyang |4 aut | |
| 700 | 1 | |a Jiang, Haoyu |4 aut | |
| 700 | 1 | |a Jing, Hantao |4 aut | |
| 700 | 1 | |a Kang, Ling |4 aut | |
| 700 | 1 | |a Kang, Mingtao |4 aut | |
| 700 | 1 | |a Li, Bo |4 aut | |
| 700 | 1 | |a Li, Lun |4 aut | |
| 700 | 1 | |a Li, Qiang |4 aut | |
| 700 | 1 | |a Li, Xiao |4 aut | |
| 700 | 1 | |a Li, Yang |4 aut | |
| 700 | 1 | |a Li, Yang |4 aut | |
| 700 | 1 | |a Liu, Rong |4 aut | |
| 700 | 1 | |a Liu, Shubin |4 aut | |
| 700 | 1 | |a Liu, Xingyan |4 aut | |
| 700 | 1 | |a Ma, Yinglin |4 aut | |
| 700 | 1 | |a Ning, Changjun |4 aut | |
| 700 | 1 | |a Qi, Binbin |4 aut | |
| 700 | 1 | |a Song, Zhaohui |4 aut | |
| 700 | 1 | |a Sun, Hong |4 aut | |
| 700 | 1 | |a Sun, Xiaoyang |4 aut | |
| 700 | 1 | |a Sun, Zhijia |4 aut | |
| 700 | 1 | |a Tan, Zhixin |4 aut | |
| 700 | 1 | |a Tang, Hongqing |4 aut | |
| 700 | 1 | |a Tang, Jingyu |4 aut | |
| 700 | 1 | |a Wang, Pengcheng |4 aut | |
| 700 | 1 | |a Wang, Qi |4 aut | |
| 700 | 1 | |a Wang, Taofeng |4 aut | |
| 700 | 1 | |a Wang, Yanfeng |4 aut | |
| 700 | 1 | |a Wang, Zhaohui |4 aut | |
| 700 | 1 | |a Wang, Zheng |4 aut | |
| 700 | 1 | |a Wen, Jie |4 aut | |
| 700 | 1 | |a Wen, Zhongwei |4 aut | |
| 700 | 1 | |a Wu, Qingbiao |4 aut | |
| 700 | 1 | |a Wu, Xiaoguang |4 aut | |
| 700 | 1 | |a Wu, Xuan |4 aut | |
| 700 | 1 | |a Xie, Likun |4 aut | |
| 700 | 1 | |a Yang, Yiwei |4 aut | |
| 700 | 1 | |a Yi, Han |4 aut | |
| 700 | 1 | |a Yu, Li |4 aut | |
| 700 | 1 | |a Yu, Tao |4 aut | |
| 700 | 1 | |a Yu, Yongji |4 aut | |
| 700 | 1 | |a Zhang, Guohui |4 aut | |
| 700 | 1 | |a Zhang, Jing |4 aut | |
| 700 | 1 | |a Zhang, Linhao |4 aut | |
| 700 | 1 | |a Zhang, Liying |4 aut | |
| 700 | 1 | |a Zhang, Qingmin |4 aut | |
| 700 | 1 | |a Zhang, Qiwei |4 aut | |
| 700 | 1 | |a Zhang, Xianpeng |4 aut | |
| 700 | 1 | |a Zhang, Yuliang |4 aut | |
| 700 | 1 | |a Zhang, Zhiyong |4 aut | |
| 700 | 1 | |a Zhao, Yingtan |4 aut | |
| 700 | 1 | |a Zhou, Liang |4 aut | |
| 700 | 1 | |a Zhou, Zuying |4 aut | |
| 700 | 1 | |a Zhu, Danyang |4 aut | |
| 700 | 1 | |a Zhu, Kejun |4 aut | |
| 700 | 1 | |a Zhu, Peng |4 aut | |
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10.1007/s41605-019-0129-8 doi (DE-627)SPR038252805 (SPR)s41605-019-0129-8-e DE-627 ger DE-627 rakwb eng Ren, Jie verfasserin (orcid)0000-0003-2738-537X aut The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Institute of High Energy Physics, Chinese Academy of Sciences; Nuclear Electronics and Nuclear Detection Society 2019 Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitivity and fast time response. The Back-n white neutron source at China Spallation Neutron Source is the first spallation white neutron source in China, and it is suitable for neutron capture cross-sectional measurement. Materials and methods A $ C_{6} %$ D_{6} $ detector system was built in the Back-n experimental station. The pulse height weighting technique was used to determine the system’s detection efficiency. The response to gamma rays of the $ C_{6} %$ D_{6} $ detector was measured, and the energy resolution function was determined. Monte Carlo simulation with Geant4 code was carried out to get the weighting function of this $ C_{6} %$ D_{6} $ detector system. Additionally, the systematic uncertainty of the weighting function was also determined. Conclusion According to the experimental and simulation results, this $ C_{6} %$ D_{6} $ detector system can be used to measure neutron capture cross section. C (dpeaa)DE-He213 D (dpeaa)DE-He213 detector (dpeaa)DE-He213 PHWT (dpeaa)DE-He213 Neutron capture cross section (dpeaa)DE-He213 White neutron source (dpeaa)DE-He213 Ruan, Xichao aut Bao, Jie aut Luan, Guangyuan aut Jiang, Wei aut An, Qi aut Bai, Huaiyong aut Cao, Ping aut Chen, Qiping aut Chen, Yonghao aut Cheng, Pinjing aut Cui, Zengqi aut Fan, Ruirui aut Feng, Changqing aut Gu, Minhao aut Guo, Fengqin aut Han, Changcai aut Han, Zijie aut He, Guozhu aut He, Yongcheng aut He, Yuefeng aut Huang, Hanxiong aut Huang, Weiling aut Huang, Xiru aut Ji, Xiaolu aut Ji, Xuyang aut Jiang, Haoyu aut Jing, Hantao aut Kang, Ling aut Kang, Mingtao aut Li, Bo aut Li, Lun aut Li, Qiang aut Li, Xiao aut Li, Yang aut Li, Yang aut Liu, Rong aut Liu, Shubin aut Liu, Xingyan aut Ma, Yinglin aut Ning, Changjun aut Qi, Binbin aut Song, Zhaohui aut Sun, Hong aut Sun, Xiaoyang aut Sun, Zhijia aut Tan, Zhixin aut Tang, Hongqing aut Tang, Jingyu aut Wang, Pengcheng aut Wang, Qi aut Wang, Taofeng aut Wang, Yanfeng aut Wang, Zhaohui aut Wang, Zheng aut Wen, Jie aut Wen, Zhongwei aut Wu, Qingbiao aut Wu, Xiaoguang aut Wu, Xuan aut Xie, Likun aut Yang, Yiwei aut Yi, Han aut Yu, Li aut Yu, Tao aut Yu, Yongji aut Zhang, Guohui aut Zhang, Jing aut Zhang, Linhao aut Zhang, Liying aut Zhang, Qingmin aut Zhang, Qiwei aut Zhang, Xianpeng aut Zhang, Yuliang aut Zhang, Zhiyong aut Zhao, Yingtan aut Zhou, Liang aut Zhou, Zuying aut Zhu, Danyang aut Zhu, Kejun aut Zhu, Peng aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 3(2019), 3 vom: 18. Juni (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:3 year:2019 number:3 day:18 month:06 https://dx.doi.org/10.1007/s41605-019-0129-8 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_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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 GBV_ILN_2118 GBV_ILN_2119 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_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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 3 2019 3 18 06 |
| spelling |
10.1007/s41605-019-0129-8 doi (DE-627)SPR038252805 (SPR)s41605-019-0129-8-e DE-627 ger DE-627 rakwb eng Ren, Jie verfasserin (orcid)0000-0003-2738-537X aut The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Institute of High Energy Physics, Chinese Academy of Sciences; Nuclear Electronics and Nuclear Detection Society 2019 Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitivity and fast time response. The Back-n white neutron source at China Spallation Neutron Source is the first spallation white neutron source in China, and it is suitable for neutron capture cross-sectional measurement. Materials and methods A $ C_{6} %$ D_{6} $ detector system was built in the Back-n experimental station. The pulse height weighting technique was used to determine the system’s detection efficiency. The response to gamma rays of the $ C_{6} %$ D_{6} $ detector was measured, and the energy resolution function was determined. Monte Carlo simulation with Geant4 code was carried out to get the weighting function of this $ C_{6} %$ D_{6} $ detector system. Additionally, the systematic uncertainty of the weighting function was also determined. Conclusion According to the experimental and simulation results, this $ C_{6} %$ D_{6} $ detector system can be used to measure neutron capture cross section. C (dpeaa)DE-He213 D (dpeaa)DE-He213 detector (dpeaa)DE-He213 PHWT (dpeaa)DE-He213 Neutron capture cross section (dpeaa)DE-He213 White neutron source (dpeaa)DE-He213 Ruan, Xichao aut Bao, Jie aut Luan, Guangyuan aut Jiang, Wei aut An, Qi aut Bai, Huaiyong aut Cao, Ping aut Chen, Qiping aut Chen, Yonghao aut Cheng, Pinjing aut Cui, Zengqi aut Fan, Ruirui aut Feng, Changqing aut Gu, Minhao aut Guo, Fengqin aut Han, Changcai aut Han, Zijie aut He, Guozhu aut He, Yongcheng aut He, Yuefeng aut Huang, Hanxiong aut Huang, Weiling aut Huang, Xiru aut Ji, Xiaolu aut Ji, Xuyang aut Jiang, Haoyu aut Jing, Hantao aut Kang, Ling aut Kang, Mingtao aut Li, Bo aut Li, Lun aut Li, Qiang aut Li, Xiao aut Li, Yang aut Li, Yang aut Liu, Rong aut Liu, Shubin aut Liu, Xingyan aut Ma, Yinglin aut Ning, Changjun aut Qi, Binbin aut Song, Zhaohui aut Sun, Hong aut Sun, Xiaoyang aut Sun, Zhijia aut Tan, Zhixin aut Tang, Hongqing aut Tang, Jingyu aut Wang, Pengcheng aut Wang, Qi aut Wang, Taofeng aut Wang, Yanfeng aut Wang, Zhaohui aut Wang, Zheng aut Wen, Jie aut Wen, Zhongwei aut Wu, Qingbiao aut Wu, Xiaoguang aut Wu, Xuan aut Xie, Likun aut Yang, Yiwei aut Yi, Han aut Yu, Li aut Yu, Tao aut Yu, Yongji aut Zhang, Guohui aut Zhang, Jing aut Zhang, Linhao aut Zhang, Liying aut Zhang, Qingmin aut Zhang, Qiwei aut Zhang, Xianpeng aut Zhang, Yuliang aut Zhang, Zhiyong aut Zhao, Yingtan aut Zhou, Liang aut Zhou, Zuying aut Zhu, Danyang aut Zhu, Kejun aut Zhu, Peng aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 3(2019), 3 vom: 18. Juni (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:3 year:2019 number:3 day:18 month:06 https://dx.doi.org/10.1007/s41605-019-0129-8 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_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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 GBV_ILN_2118 GBV_ILN_2119 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_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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 3 2019 3 18 06 |
| allfields_unstemmed |
10.1007/s41605-019-0129-8 doi (DE-627)SPR038252805 (SPR)s41605-019-0129-8-e DE-627 ger DE-627 rakwb eng Ren, Jie verfasserin (orcid)0000-0003-2738-537X aut The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Institute of High Energy Physics, Chinese Academy of Sciences; Nuclear Electronics and Nuclear Detection Society 2019 Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitivity and fast time response. The Back-n white neutron source at China Spallation Neutron Source is the first spallation white neutron source in China, and it is suitable for neutron capture cross-sectional measurement. Materials and methods A $ C_{6} %$ D_{6} $ detector system was built in the Back-n experimental station. The pulse height weighting technique was used to determine the system’s detection efficiency. The response to gamma rays of the $ C_{6} %$ D_{6} $ detector was measured, and the energy resolution function was determined. Monte Carlo simulation with Geant4 code was carried out to get the weighting function of this $ C_{6} %$ D_{6} $ detector system. Additionally, the systematic uncertainty of the weighting function was also determined. Conclusion According to the experimental and simulation results, this $ C_{6} %$ D_{6} $ detector system can be used to measure neutron capture cross section. C (dpeaa)DE-He213 D (dpeaa)DE-He213 detector (dpeaa)DE-He213 PHWT (dpeaa)DE-He213 Neutron capture cross section (dpeaa)DE-He213 White neutron source (dpeaa)DE-He213 Ruan, Xichao aut Bao, Jie aut Luan, Guangyuan aut Jiang, Wei aut An, Qi aut Bai, Huaiyong aut Cao, Ping aut Chen, Qiping aut Chen, Yonghao aut Cheng, Pinjing aut Cui, Zengqi aut Fan, Ruirui aut Feng, Changqing aut Gu, Minhao aut Guo, Fengqin aut Han, Changcai aut Han, Zijie aut He, Guozhu aut He, Yongcheng aut He, Yuefeng aut Huang, Hanxiong aut Huang, Weiling aut Huang, Xiru aut Ji, Xiaolu aut Ji, Xuyang aut Jiang, Haoyu aut Jing, Hantao aut Kang, Ling aut Kang, Mingtao aut Li, Bo aut Li, Lun aut Li, Qiang aut Li, Xiao aut Li, Yang aut Li, Yang aut Liu, Rong aut Liu, Shubin aut Liu, Xingyan aut Ma, Yinglin aut Ning, Changjun aut Qi, Binbin aut Song, Zhaohui aut Sun, Hong aut Sun, Xiaoyang aut Sun, Zhijia aut Tan, Zhixin aut Tang, Hongqing aut Tang, Jingyu aut Wang, Pengcheng aut Wang, Qi aut Wang, Taofeng aut Wang, Yanfeng aut Wang, Zhaohui aut Wang, Zheng aut Wen, Jie aut Wen, Zhongwei aut Wu, Qingbiao aut Wu, Xiaoguang aut Wu, Xuan aut Xie, Likun aut Yang, Yiwei aut Yi, Han aut Yu, Li aut Yu, Tao aut Yu, Yongji aut Zhang, Guohui aut Zhang, Jing aut Zhang, Linhao aut Zhang, Liying aut Zhang, Qingmin aut Zhang, Qiwei aut Zhang, Xianpeng aut Zhang, Yuliang aut Zhang, Zhiyong aut Zhao, Yingtan aut Zhou, Liang aut Zhou, Zuying aut Zhu, Danyang aut Zhu, Kejun aut Zhu, Peng aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 3(2019), 3 vom: 18. Juni (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:3 year:2019 number:3 day:18 month:06 https://dx.doi.org/10.1007/s41605-019-0129-8 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_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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 GBV_ILN_2118 GBV_ILN_2119 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_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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 3 2019 3 18 06 |
| allfieldsGer |
10.1007/s41605-019-0129-8 doi (DE-627)SPR038252805 (SPR)s41605-019-0129-8-e DE-627 ger DE-627 rakwb eng Ren, Jie verfasserin (orcid)0000-0003-2738-537X aut The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Institute of High Energy Physics, Chinese Academy of Sciences; Nuclear Electronics and Nuclear Detection Society 2019 Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitivity and fast time response. The Back-n white neutron source at China Spallation Neutron Source is the first spallation white neutron source in China, and it is suitable for neutron capture cross-sectional measurement. Materials and methods A $ C_{6} %$ D_{6} $ detector system was built in the Back-n experimental station. The pulse height weighting technique was used to determine the system’s detection efficiency. The response to gamma rays of the $ C_{6} %$ D_{6} $ detector was measured, and the energy resolution function was determined. Monte Carlo simulation with Geant4 code was carried out to get the weighting function of this $ C_{6} %$ D_{6} $ detector system. Additionally, the systematic uncertainty of the weighting function was also determined. Conclusion According to the experimental and simulation results, this $ C_{6} %$ D_{6} $ detector system can be used to measure neutron capture cross section. C (dpeaa)DE-He213 D (dpeaa)DE-He213 detector (dpeaa)DE-He213 PHWT (dpeaa)DE-He213 Neutron capture cross section (dpeaa)DE-He213 White neutron source (dpeaa)DE-He213 Ruan, Xichao aut Bao, Jie aut Luan, Guangyuan aut Jiang, Wei aut An, Qi aut Bai, Huaiyong aut Cao, Ping aut Chen, Qiping aut Chen, Yonghao aut Cheng, Pinjing aut Cui, Zengqi aut Fan, Ruirui aut Feng, Changqing aut Gu, Minhao aut Guo, Fengqin aut Han, Changcai aut Han, Zijie aut He, Guozhu aut He, Yongcheng aut He, Yuefeng aut Huang, Hanxiong aut Huang, Weiling aut Huang, Xiru aut Ji, Xiaolu aut Ji, Xuyang aut Jiang, Haoyu aut Jing, Hantao aut Kang, Ling aut Kang, Mingtao aut Li, Bo aut Li, Lun aut Li, Qiang aut Li, Xiao aut Li, Yang aut Li, Yang aut Liu, Rong aut Liu, Shubin aut Liu, Xingyan aut Ma, Yinglin aut Ning, Changjun aut Qi, Binbin aut Song, Zhaohui aut Sun, Hong aut Sun, Xiaoyang aut Sun, Zhijia aut Tan, Zhixin aut Tang, Hongqing aut Tang, Jingyu aut Wang, Pengcheng aut Wang, Qi aut Wang, Taofeng aut Wang, Yanfeng aut Wang, Zhaohui aut Wang, Zheng aut Wen, Jie aut Wen, Zhongwei aut Wu, Qingbiao aut Wu, Xiaoguang aut Wu, Xuan aut Xie, Likun aut Yang, Yiwei aut Yi, Han aut Yu, Li aut Yu, Tao aut Yu, Yongji aut Zhang, Guohui aut Zhang, Jing aut Zhang, Linhao aut Zhang, Liying aut Zhang, Qingmin aut Zhang, Qiwei aut Zhang, Xianpeng aut Zhang, Yuliang aut Zhang, Zhiyong aut Zhao, Yingtan aut Zhou, Liang aut Zhou, Zuying aut Zhu, Danyang aut Zhu, Kejun aut Zhu, Peng aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 3(2019), 3 vom: 18. Juni (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:3 year:2019 number:3 day:18 month:06 https://dx.doi.org/10.1007/s41605-019-0129-8 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_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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 GBV_ILN_2118 GBV_ILN_2119 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_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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 3 2019 3 18 06 |
| allfieldsSound |
10.1007/s41605-019-0129-8 doi (DE-627)SPR038252805 (SPR)s41605-019-0129-8-e DE-627 ger DE-627 rakwb eng Ren, Jie verfasserin (orcid)0000-0003-2738-537X aut The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Institute of High Energy Physics, Chinese Academy of Sciences; Nuclear Electronics and Nuclear Detection Society 2019 Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitivity and fast time response. The Back-n white neutron source at China Spallation Neutron Source is the first spallation white neutron source in China, and it is suitable for neutron capture cross-sectional measurement. Materials and methods A $ C_{6} %$ D_{6} $ detector system was built in the Back-n experimental station. The pulse height weighting technique was used to determine the system’s detection efficiency. The response to gamma rays of the $ C_{6} %$ D_{6} $ detector was measured, and the energy resolution function was determined. Monte Carlo simulation with Geant4 code was carried out to get the weighting function of this $ C_{6} %$ D_{6} $ detector system. Additionally, the systematic uncertainty of the weighting function was also determined. Conclusion According to the experimental and simulation results, this $ C_{6} %$ D_{6} $ detector system can be used to measure neutron capture cross section. C (dpeaa)DE-He213 D (dpeaa)DE-He213 detector (dpeaa)DE-He213 PHWT (dpeaa)DE-He213 Neutron capture cross section (dpeaa)DE-He213 White neutron source (dpeaa)DE-He213 Ruan, Xichao aut Bao, Jie aut Luan, Guangyuan aut Jiang, Wei aut An, Qi aut Bai, Huaiyong aut Cao, Ping aut Chen, Qiping aut Chen, Yonghao aut Cheng, Pinjing aut Cui, Zengqi aut Fan, Ruirui aut Feng, Changqing aut Gu, Minhao aut Guo, Fengqin aut Han, Changcai aut Han, Zijie aut He, Guozhu aut He, Yongcheng aut He, Yuefeng aut Huang, Hanxiong aut Huang, Weiling aut Huang, Xiru aut Ji, Xiaolu aut Ji, Xuyang aut Jiang, Haoyu aut Jing, Hantao aut Kang, Ling aut Kang, Mingtao aut Li, Bo aut Li, Lun aut Li, Qiang aut Li, Xiao aut Li, Yang aut Li, Yang aut Liu, Rong aut Liu, Shubin aut Liu, Xingyan aut Ma, Yinglin aut Ning, Changjun aut Qi, Binbin aut Song, Zhaohui aut Sun, Hong aut Sun, Xiaoyang aut Sun, Zhijia aut Tan, Zhixin aut Tang, Hongqing aut Tang, Jingyu aut Wang, Pengcheng aut Wang, Qi aut Wang, Taofeng aut Wang, Yanfeng aut Wang, Zhaohui aut Wang, Zheng aut Wen, Jie aut Wen, Zhongwei aut Wu, Qingbiao aut Wu, Xiaoguang aut Wu, Xuan aut Xie, Likun aut Yang, Yiwei aut Yi, Han aut Yu, Li aut Yu, Tao aut Yu, Yongji aut Zhang, Guohui aut Zhang, Jing aut Zhang, Linhao aut Zhang, Liying aut Zhang, Qingmin aut Zhang, Qiwei aut Zhang, Xianpeng aut Zhang, Yuliang aut Zhang, Zhiyong aut Zhao, Yingtan aut Zhou, Liang aut Zhou, Zuying aut Zhu, Danyang aut Zhu, Kejun aut Zhu, Peng aut Enthalten in Radiation detection technology and methods [Singapore] : Springer Singapore, 2017 3(2019), 3 vom: 18. Juni (DE-627)886059038 (DE-600)2893569-X 2509-9949 nnns volume:3 year:2019 number:3 day:18 month:06 https://dx.doi.org/10.1007/s41605-019-0129-8 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_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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 GBV_ILN_2118 GBV_ILN_2119 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_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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 3 2019 3 18 06 |
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English |
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Enthalten in Radiation detection technology and methods 3(2019), 3 vom: 18. Juni volume:3 year:2019 number:3 day:18 month:06 |
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Enthalten in Radiation detection technology and methods 3(2019), 3 vom: 18. Juni volume:3 year:2019 number:3 day:18 month:06 |
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Article |
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C D detector PHWT Neutron capture cross section White neutron source |
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Radiation detection technology and methods |
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Ren, Jie @@aut@@ Ruan, Xichao @@aut@@ Bao, Jie @@aut@@ Luan, Guangyuan @@aut@@ Jiang, Wei @@aut@@ An, Qi @@aut@@ Bai, Huaiyong @@aut@@ Cao, Ping @@aut@@ Chen, Qiping @@aut@@ Chen, Yonghao @@aut@@ Cheng, Pinjing @@aut@@ Cui, Zengqi @@aut@@ Fan, Ruirui @@aut@@ Feng, Changqing @@aut@@ Gu, Minhao @@aut@@ Guo, Fengqin @@aut@@ Han, Changcai @@aut@@ Han, Zijie @@aut@@ He, Guozhu @@aut@@ He, Yongcheng @@aut@@ He, Yuefeng @@aut@@ Huang, Hanxiong @@aut@@ Huang, Weiling @@aut@@ Huang, Xiru @@aut@@ Ji, Xiaolu @@aut@@ Ji, Xuyang @@aut@@ Jiang, Haoyu @@aut@@ Jing, Hantao @@aut@@ Kang, Ling @@aut@@ Kang, Mingtao @@aut@@ Li, Bo @@aut@@ Li, Lun @@aut@@ Li, Qiang @@aut@@ Li, Xiao @@aut@@ Li, Yang @@aut@@ Liu, Rong @@aut@@ Liu, Shubin @@aut@@ Liu, Xingyan @@aut@@ Ma, Yinglin @@aut@@ Ning, Changjun @@aut@@ Qi, Binbin @@aut@@ Song, Zhaohui @@aut@@ Sun, Hong @@aut@@ Sun, Xiaoyang @@aut@@ Sun, Zhijia @@aut@@ Tan, Zhixin @@aut@@ Tang, Hongqing @@aut@@ Tang, Jingyu @@aut@@ Wang, Pengcheng @@aut@@ Wang, Qi @@aut@@ Wang, Taofeng @@aut@@ Wang, Yanfeng @@aut@@ Wang, Zhaohui @@aut@@ Wang, Zheng @@aut@@ Wen, Jie @@aut@@ Wen, Zhongwei @@aut@@ Wu, Qingbiao @@aut@@ Wu, Xiaoguang @@aut@@ Wu, Xuan @@aut@@ Xie, Likun @@aut@@ Yang, Yiwei @@aut@@ Yi, Han @@aut@@ Yu, Li @@aut@@ Yu, Tao @@aut@@ Yu, Yongji @@aut@@ Zhang, Guohui @@aut@@ Zhang, Jing @@aut@@ Zhang, Linhao @@aut@@ Zhang, Liying @@aut@@ Zhang, Qingmin @@aut@@ Zhang, Qiwei @@aut@@ Zhang, Xianpeng @@aut@@ Zhang, Yuliang @@aut@@ Zhang, Zhiyong @@aut@@ Zhao, Yingtan @@aut@@ Zhou, Liang @@aut@@ Zhou, Zuying @@aut@@ Zhu, Danyang @@aut@@ Zhu, Kejun @@aut@@ Zhu, Peng @@aut@@ |
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2019-06-18T00:00:00Z |
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SPR038252805 |
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englisch |
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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">SPR038252805</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230328195929.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201007s2019 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s41605-019-0129-8</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR038252805</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s41605-019-0129-8-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">Ren, Jie</subfield><subfield code="e">verfasserin</subfield><subfield code="0">(orcid)0000-0003-2738-537X</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="4"><subfield code="a">The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2019</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; Nuclear Electronics and Nuclear Detection Society 2019</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitivity and fast time response. The Back-n white neutron source at China Spallation Neutron Source is the first spallation white neutron source in China, and it is suitable for neutron capture cross-sectional measurement. Materials and methods A $ C_{6} %$ D_{6} $ detector system was built in the Back-n experimental station. The pulse height weighting technique was used to determine the system’s detection efficiency. The response to gamma rays of the $ C_{6} %$ D_{6} $ detector was measured, and the energy resolution function was determined. Monte Carlo simulation with Geant4 code was carried out to get the weighting function of this $ C_{6} %$ D_{6} $ detector system. Additionally, the systematic uncertainty of the weighting function was also determined. 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Ren, Jie |
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The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS C (dpeaa)DE-He213 D (dpeaa)DE-He213 detector (dpeaa)DE-He213 PHWT (dpeaa)DE-He213 Neutron capture cross section (dpeaa)DE-He213 White neutron source (dpeaa)DE-He213 |
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The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS |
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Ren, Jie Ruan, Xichao Bao, Jie Luan, Guangyuan Jiang, Wei An, Qi Bai, Huaiyong Cao, Ping Chen, Qiping Chen, Yonghao Cheng, Pinjing Cui, Zengqi Fan, Ruirui Feng, Changqing Gu, Minhao Guo, Fengqin Han, Changcai Han, Zijie He, Guozhu He, Yongcheng He, Yuefeng Huang, Hanxiong Huang, Weiling Huang, Xiru Ji, Xiaolu Ji, Xuyang Jiang, Haoyu Jing, Hantao Kang, Ling Kang, Mingtao Li, Bo Li, Lun Li, Qiang Li, Xiao Li, Yang Liu, Rong Liu, Shubin Liu, Xingyan Ma, Yinglin Ning, Changjun Qi, Binbin Song, Zhaohui Sun, Hong Sun, Xiaoyang Sun, Zhijia Tan, Zhixin Tang, Hongqing Tang, Jingyu Wang, Pengcheng Wang, Qi Wang, Taofeng Wang, Yanfeng Wang, Zhaohui Wang, Zheng Wen, Jie Wen, Zhongwei Wu, Qingbiao Wu, Xiaoguang Wu, Xuan Xie, Likun Yang, Yiwei Yi, Han Yu, Li Yu, Tao Yu, Yongji Zhang, Guohui Zhang, Jing Zhang, Linhao Zhang, Liying Zhang, Qingmin Zhang, Qiwei Zhang, Xianpeng Zhang, Yuliang Zhang, Zhiyong Zhao, Yingtan Zhou, Liang Zhou, Zuying Zhu, Danyang Zhu, Kejun Zhu, Peng |
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Elektronische Aufsätze |
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Ren, Jie |
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10.1007/s41605-019-0129-8 |
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$ c_{6} %$ d_{6} $ detector system on the back-n beam line of csns |
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The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS |
| abstract |
Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitivity and fast time response. The Back-n white neutron source at China Spallation Neutron Source is the first spallation white neutron source in China, and it is suitable for neutron capture cross-sectional measurement. Materials and methods A $ C_{6} %$ D_{6} $ detector system was built in the Back-n experimental station. The pulse height weighting technique was used to determine the system’s detection efficiency. The response to gamma rays of the $ C_{6} %$ D_{6} $ detector was measured, and the energy resolution function was determined. Monte Carlo simulation with Geant4 code was carried out to get the weighting function of this $ C_{6} %$ D_{6} $ detector system. Additionally, the systematic uncertainty of the weighting function was also determined. Conclusion According to the experimental and simulation results, this $ C_{6} %$ D_{6} $ detector system can be used to measure neutron capture cross section. © Institute of High Energy Physics, Chinese Academy of Sciences; Nuclear Electronics and Nuclear Detection Society 2019 |
| abstractGer |
Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitivity and fast time response. The Back-n white neutron source at China Spallation Neutron Source is the first spallation white neutron source in China, and it is suitable for neutron capture cross-sectional measurement. Materials and methods A $ C_{6} %$ D_{6} $ detector system was built in the Back-n experimental station. The pulse height weighting technique was used to determine the system’s detection efficiency. The response to gamma rays of the $ C_{6} %$ D_{6} $ detector was measured, and the energy resolution function was determined. Monte Carlo simulation with Geant4 code was carried out to get the weighting function of this $ C_{6} %$ D_{6} $ detector system. Additionally, the systematic uncertainty of the weighting function was also determined. Conclusion According to the experimental and simulation results, this $ C_{6} %$ D_{6} $ detector system can be used to measure neutron capture cross section. © Institute of High Energy Physics, Chinese Academy of Sciences; Nuclear Electronics and Nuclear Detection Society 2019 |
| abstract_unstemmed |
Introduction The neutron capture cross sections are very important in the field of nuclear device design and basic physics research. Hydrogen-free liquid scintillator such as $ C_{6} %$ D_{6} $ detectors are widely used in the neutron capture cross-sectional measurements for the low neutron sensitivity and fast time response. The Back-n white neutron source at China Spallation Neutron Source is the first spallation white neutron source in China, and it is suitable for neutron capture cross-sectional measurement. Materials and methods A $ C_{6} %$ D_{6} $ detector system was built in the Back-n experimental station. The pulse height weighting technique was used to determine the system’s detection efficiency. The response to gamma rays of the $ C_{6} %$ D_{6} $ detector was measured, and the energy resolution function was determined. Monte Carlo simulation with Geant4 code was carried out to get the weighting function of this $ C_{6} %$ D_{6} $ detector system. Additionally, the systematic uncertainty of the weighting function was also determined. Conclusion According to the experimental and simulation results, this $ C_{6} %$ D_{6} $ detector system can be used to measure neutron capture cross section. © Institute of High Energy Physics, Chinese Academy of Sciences; Nuclear Electronics and Nuclear Detection Society 2019 |
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The $ C_{6} %$ D_{6} $ detector system on the Back-n beam line of CSNS |
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https://dx.doi.org/10.1007/s41605-019-0129-8 |
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Ruan, Xichao Bao, Jie Luan, Guangyuan Jiang, Wei An, Qi Bai, Huaiyong Cao, Ping Chen, Qiping Chen, Yonghao Cheng, Pinjing Cui, Zengqi Fan, Ruirui Feng, Changqing Gu, Minhao Guo, Fengqin Han, Changcai Han, Zijie He, Guozhu He, Yongcheng He, Yuefeng Huang, Hanxiong Huang, Weiling Huang, Xiru Ji, Xiaolu Ji, Xuyang Jiang, Haoyu Jing, Hantao Kang, Ling Kang, Mingtao Li, Bo Li, Lun Li, Qiang Li, Xiao Li, Yang Liu, Rong Liu, Shubin Liu, Xingyan Ma, Yinglin Ning, Changjun Qi, Binbin Song, Zhaohui Sun, Hong Sun, Xiaoyang Sun, Zhijia Tan, Zhixin Tang, Hongqing Tang, Jingyu Wang, Pengcheng Wang, Qi Wang, Taofeng Wang, Yanfeng Wang, Zhaohui Wang, Zheng Wen, Jie Wen, Zhongwei Wu, Qingbiao Wu, Xiaoguang Wu, Xuan Xie, Likun Yang, Yiwei Yi, Han Yu, Li Yu, Tao Yu, Yongji Zhang, Guohui Zhang, Jing Zhang, Linhao Zhang, Liying Zhang, Qingmin Zhang, Qiwei Zhang, Xianpeng Zhang, Yuliang Zhang, Zhiyong Zhao, Yingtan Zhou, Liang Zhou, Zuying Zhu, Danyang Zhu, Kejun Zhu, Peng |
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Ruan, Xichao Bao, Jie Luan, Guangyuan Jiang, Wei An, Qi Bai, Huaiyong Cao, Ping Chen, Qiping Chen, Yonghao Cheng, Pinjing Cui, Zengqi Fan, Ruirui Feng, Changqing Gu, Minhao Guo, Fengqin Han, Changcai Han, Zijie He, Guozhu He, Yongcheng He, Yuefeng Huang, Hanxiong Huang, Weiling Huang, Xiru Ji, Xiaolu Ji, Xuyang Jiang, Haoyu Jing, Hantao Kang, Ling Kang, Mingtao Li, Bo Li, Lun Li, Qiang Li, Xiao Li, Yang Liu, Rong Liu, Shubin Liu, Xingyan Ma, Yinglin Ning, Changjun Qi, Binbin Song, Zhaohui Sun, Hong Sun, Xiaoyang Sun, Zhijia Tan, Zhixin Tang, Hongqing Tang, Jingyu Wang, Pengcheng Wang, Qi Wang, Taofeng Wang, Yanfeng Wang, Zhaohui Wang, Zheng Wen, Jie Wen, Zhongwei Wu, Qingbiao Wu, Xiaoguang Wu, Xuan Xie, Likun Yang, Yiwei Yi, Han Yu, Li Yu, Tao Yu, Yongji Zhang, Guohui Zhang, Jing Zhang, Linhao Zhang, Liying Zhang, Qingmin Zhang, Qiwei Zhang, Xianpeng Zhang, Yuliang Zhang, Zhiyong Zhao, Yingtan Zhou, Liang Zhou, Zuying Zhu, Danyang Zhu, Kejun Zhu, Peng |
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2024-07-03T17:00:56.028Z |
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7.401288 |