Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS
Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neut...
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| Autor*in: |
Liu, Xingyan [verfasserIn] Yang, Yiwei [verfasserIn] Liu, Rong [verfasserIn] Wen, Zhongwei [verfasserIn] Wen, Jie [verfasserIn] Han, Zijie [verfasserIn] Chen, Yonghao [verfasserIn] Jing, Hantao [verfasserIn] Yi, Han [verfasserIn] Bao, Jie [verfasserIn] Ren, Zhizhou [verfasserIn] An, Qi [verfasserIn] Bai, Huaiyong [verfasserIn] Cao, Ping [verfasserIn] Chen, Qiping [verfasserIn] Cheng, Pinjing [verfasserIn] Cui, Zengqi [verfasserIn] Fan, Ruirui [verfasserIn] Feng, Changqing [verfasserIn] Gu, Minhao [verfasserIn] Guo, Fengqin [verfasserIn] Han, Changcai [verfasserIn] He, Guozhu [verfasserIn] He, Yongcheng [verfasserIn] He, Yuefeng [verfasserIn] Huang, Hanxiong [verfasserIn] Huang, Weiling [verfasserIn] Huang, Xiru [verfasserIn] Ji, Xiaolu [verfasserIn] Ji, Xuyang [verfasserIn] Jiang, Haoyu [verfasserIn] Jiang, Wei [verfasserIn] Kang, Ling [verfasserIn] Kang, Mingtao [verfasserIn] Li, Bo [verfasserIn] Li, Lun [verfasserIn] Li, Qiang [verfasserIn] Li, Xiao [verfasserIn] Li, Yang [verfasserIn] Liu, Shubin [verfasserIn] Luan, Guangyuan [verfasserIn] Ma, Yinglin [verfasserIn] Ning, Changjun [verfasserIn] Qi, Binbin [verfasserIn] Ren, Jie [verfasserIn] Ruan, Xichao [verfasserIn] Song, Zhaohui [verfasserIn] Sun, Hong [verfasserIn] Sun, Xiaoyang [verfasserIn] Sun, Zhijia [verfasserIn] Tan, Zhixin [verfasserIn] Tang, Hongqing [verfasserIn] Tang, Jingyu [verfasserIn] Wang, Pengcheng [verfasserIn] Wang, Qi [verfasserIn] Wang, Taofeng [verfasserIn] Wang, Yanfeng [verfasserIn] Wang, Zhaohui [verfasserIn] Wang, Zheng [verfasserIn] Wu, Qingbiao [verfasserIn] Wu, Xiaoguang [verfasserIn] Wu, Xuan [verfasserIn] Xie, Likun [verfasserIn] Yu, Li [verfasserIn] Yu, Tao [verfasserIn] Yu, Yongji [verfasserIn] Zhang, Guohui [verfasserIn] Zhang, Jing [verfasserIn] Zhang, Linhao [verfasserIn] Zhang, Liying [verfasserIn] Zhang, Qingmin [verfasserIn] Zhang, Qiwei [verfasserIn] Zhang, Xianpeng [verfasserIn] Zhang, Yuliang [verfasserIn] Zhang, Zhiyong [verfasserIn] Zhao, Yingtan [verfasserIn] Zhou, Liang [verfasserIn] Zhou, Zuying [verfasserIn] Zhu, Danyang [verfasserIn] Zhu, Kejun [verfasserIn] Zhu, Peng [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2021 |
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| Anmerkung: |
© The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021 |
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| Übergeordnetes Werk: |
Enthalten in: The European physical journal - Berlin : Springer, 1998, 57(2021), 7 vom: Juli |
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| Übergeordnetes Werk: |
volume:57 ; year:2021 ; number:7 ; month:07 |
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| DOI / URN: |
10.1140/epja/s10050-021-00513-9 |
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| Katalog-ID: |
SPR044545207 |
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| 100 | 1 | |a Liu, Xingyan |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS |
| 264 | 1 | |c 2021 | |
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| 500 | |a © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021 | ||
| 520 | |a Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neutron Source of CSNS. Two aluminum samples 70 mm in diameter and thicknesses of 40 and 60 mm, respectively, were positioned at 55 m from the neutron source. The transmission detector consisted of a multi-layer fast fission chamber loaded with %$^{235}%$U and %$^{238}%$U, and it was located at the 76-m measurement station. By applying the time-of-flight technique, it was possible to extract the n+%$^{27}%$Al total cross section in a wide energy region, from 1 eV to 20 MeV, after the correction for the double-bunch mode of the CSNS accelerator. The total cross sections obtained with the two Al samples are consistent and the results obtained with the %$^{235}%$U fission cells are in good agreement with that with %$^{238}%$U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with %$^{235}%$U for 40 mm and 60 mm thick aluminum is 0.7–22.3% and 0.6–12.4% in the energy range of 10 keV–20 MeV. Results are in fair agreement with respect to previous data and evaluations. | ||
| 700 | 1 | |a Yang, Yiwei |e verfasserin |4 aut | |
| 700 | 1 | |a Liu, Rong |e verfasserin |4 aut | |
| 700 | 1 | |a Wen, Zhongwei |e verfasserin |4 aut | |
| 700 | 1 | |a Wen, Jie |e verfasserin |4 aut | |
| 700 | 1 | |a Han, Zijie |e verfasserin |4 aut | |
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| 700 | 1 | |a Li, Yang |e verfasserin |4 aut | |
| 700 | 1 | |a Liu, Shubin |e verfasserin |4 aut | |
| 700 | 1 | |a Luan, Guangyuan |e verfasserin |4 aut | |
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| 700 | 1 | |a Ruan, Xichao |e verfasserin |4 aut | |
| 700 | 1 | |a Song, Zhaohui |e verfasserin |4 aut | |
| 700 | 1 | |a Sun, Hong |e verfasserin |4 aut | |
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10.1140/epja/s10050-021-00513-9 doi (DE-627)SPR044545207 (SPR)s10050-021-00513-9-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Liu, Xingyan verfasserin aut Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021 Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neutron Source of CSNS. Two aluminum samples 70 mm in diameter and thicknesses of 40 and 60 mm, respectively, were positioned at 55 m from the neutron source. The transmission detector consisted of a multi-layer fast fission chamber loaded with %$^{235}%$U and %$^{238}%$U, and it was located at the 76-m measurement station. By applying the time-of-flight technique, it was possible to extract the n+%$^{27}%$Al total cross section in a wide energy region, from 1 eV to 20 MeV, after the correction for the double-bunch mode of the CSNS accelerator. The total cross sections obtained with the two Al samples are consistent and the results obtained with the %$^{235}%$U fission cells are in good agreement with that with %$^{238}%$U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with %$^{235}%$U for 40 mm and 60 mm thick aluminum is 0.7–22.3% and 0.6–12.4% in the energy range of 10 keV–20 MeV. Results are in fair agreement with respect to previous data and evaluations. Yang, Yiwei verfasserin aut Liu, Rong verfasserin aut Wen, Zhongwei verfasserin aut Wen, Jie verfasserin aut Han, Zijie verfasserin aut Chen, Yonghao verfasserin aut Jing, Hantao verfasserin aut Yi, Han verfasserin aut Bao, Jie verfasserin aut Ren, Zhizhou verfasserin aut An, Qi verfasserin aut Bai, Huaiyong verfasserin aut Cao, Ping verfasserin aut Chen, Qiping verfasserin aut Cheng, Pinjing verfasserin aut Cui, Zengqi verfasserin aut Fan, Ruirui verfasserin aut Feng, Changqing verfasserin aut Gu, Minhao verfasserin aut Guo, Fengqin verfasserin aut Han, Changcai verfasserin aut He, Guozhu verfasserin aut He, Yongcheng verfasserin aut He, Yuefeng verfasserin aut Huang, Hanxiong verfasserin aut Huang, Weiling verfasserin aut Huang, Xiru verfasserin aut Ji, Xiaolu verfasserin aut Ji, Xuyang verfasserin aut Jiang, Haoyu verfasserin aut Jiang, Wei verfasserin aut Kang, Ling verfasserin aut Kang, Mingtao verfasserin aut Li, Bo verfasserin aut Li, Lun verfasserin aut Li, Qiang verfasserin aut Li, Xiao verfasserin aut Li, Yang verfasserin aut Li, Yang verfasserin aut Liu, Shubin verfasserin aut Luan, Guangyuan verfasserin aut Ma, Yinglin verfasserin aut Ning, Changjun verfasserin aut Qi, Binbin verfasserin aut Ren, Jie verfasserin aut Ruan, Xichao verfasserin aut Song, Zhaohui verfasserin aut Sun, Hong verfasserin aut Sun, Xiaoyang verfasserin aut Sun, Zhijia verfasserin aut Tan, Zhixin verfasserin aut Tang, Hongqing verfasserin aut Tang, Jingyu verfasserin aut Wang, Pengcheng verfasserin aut Wang, Qi verfasserin aut Wang, Taofeng verfasserin aut Wang, Yanfeng verfasserin aut Wang, Zhaohui verfasserin aut Wang, Zheng verfasserin aut Wu, Qingbiao verfasserin aut Wu, Xiaoguang verfasserin aut Wu, Xuan verfasserin aut Xie, Likun verfasserin aut Yu, Li verfasserin aut Yu, Tao verfasserin aut Yu, Yongji verfasserin aut Zhang, Guohui verfasserin aut Zhang, Jing verfasserin aut Zhang, Linhao verfasserin aut Zhang, Liying verfasserin aut Zhang, Qingmin verfasserin aut Zhang, Qiwei verfasserin aut Zhang, Xianpeng verfasserin aut Zhang, Yuliang verfasserin aut Zhang, Zhiyong verfasserin aut Zhao, Yingtan verfasserin aut Zhou, Liang verfasserin aut Zhou, Zuying verfasserin aut Zhu, Danyang verfasserin aut Zhu, Kejun verfasserin aut Zhu, Peng verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 57(2021), 7 vom: Juli (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:57 year:2021 number:7 month:07 https://dx.doi.org/10.1140/epja/s10050-021-00513-9 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_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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_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_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 33.40 ASE 33.50 ASE AR 57 2021 7 07 |
| spelling |
10.1140/epja/s10050-021-00513-9 doi (DE-627)SPR044545207 (SPR)s10050-021-00513-9-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Liu, Xingyan verfasserin aut Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021 Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neutron Source of CSNS. Two aluminum samples 70 mm in diameter and thicknesses of 40 and 60 mm, respectively, were positioned at 55 m from the neutron source. The transmission detector consisted of a multi-layer fast fission chamber loaded with %$^{235}%$U and %$^{238}%$U, and it was located at the 76-m measurement station. By applying the time-of-flight technique, it was possible to extract the n+%$^{27}%$Al total cross section in a wide energy region, from 1 eV to 20 MeV, after the correction for the double-bunch mode of the CSNS accelerator. The total cross sections obtained with the two Al samples are consistent and the results obtained with the %$^{235}%$U fission cells are in good agreement with that with %$^{238}%$U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with %$^{235}%$U for 40 mm and 60 mm thick aluminum is 0.7–22.3% and 0.6–12.4% in the energy range of 10 keV–20 MeV. Results are in fair agreement with respect to previous data and evaluations. Yang, Yiwei verfasserin aut Liu, Rong verfasserin aut Wen, Zhongwei verfasserin aut Wen, Jie verfasserin aut Han, Zijie verfasserin aut Chen, Yonghao verfasserin aut Jing, Hantao verfasserin aut Yi, Han verfasserin aut Bao, Jie verfasserin aut Ren, Zhizhou verfasserin aut An, Qi verfasserin aut Bai, Huaiyong verfasserin aut Cao, Ping verfasserin aut Chen, Qiping verfasserin aut Cheng, Pinjing verfasserin aut Cui, Zengqi verfasserin aut Fan, Ruirui verfasserin aut Feng, Changqing verfasserin aut Gu, Minhao verfasserin aut Guo, Fengqin verfasserin aut Han, Changcai verfasserin aut He, Guozhu verfasserin aut He, Yongcheng verfasserin aut He, Yuefeng verfasserin aut Huang, Hanxiong verfasserin aut Huang, Weiling verfasserin aut Huang, Xiru verfasserin aut Ji, Xiaolu verfasserin aut Ji, Xuyang verfasserin aut Jiang, Haoyu verfasserin aut Jiang, Wei verfasserin aut Kang, Ling verfasserin aut Kang, Mingtao verfasserin aut Li, Bo verfasserin aut Li, Lun verfasserin aut Li, Qiang verfasserin aut Li, Xiao verfasserin aut Li, Yang verfasserin aut Li, Yang verfasserin aut Liu, Shubin verfasserin aut Luan, Guangyuan verfasserin aut Ma, Yinglin verfasserin aut Ning, Changjun verfasserin aut Qi, Binbin verfasserin aut Ren, Jie verfasserin aut Ruan, Xichao verfasserin aut Song, Zhaohui verfasserin aut Sun, Hong verfasserin aut Sun, Xiaoyang verfasserin aut Sun, Zhijia verfasserin aut Tan, Zhixin verfasserin aut Tang, Hongqing verfasserin aut Tang, Jingyu verfasserin aut Wang, Pengcheng verfasserin aut Wang, Qi verfasserin aut Wang, Taofeng verfasserin aut Wang, Yanfeng verfasserin aut Wang, Zhaohui verfasserin aut Wang, Zheng verfasserin aut Wu, Qingbiao verfasserin aut Wu, Xiaoguang verfasserin aut Wu, Xuan verfasserin aut Xie, Likun verfasserin aut Yu, Li verfasserin aut Yu, Tao verfasserin aut Yu, Yongji verfasserin aut Zhang, Guohui verfasserin aut Zhang, Jing verfasserin aut Zhang, Linhao verfasserin aut Zhang, Liying verfasserin aut Zhang, Qingmin verfasserin aut Zhang, Qiwei verfasserin aut Zhang, Xianpeng verfasserin aut Zhang, Yuliang verfasserin aut Zhang, Zhiyong verfasserin aut Zhao, Yingtan verfasserin aut Zhou, Liang verfasserin aut Zhou, Zuying verfasserin aut Zhu, Danyang verfasserin aut Zhu, Kejun verfasserin aut Zhu, Peng verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 57(2021), 7 vom: Juli (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:57 year:2021 number:7 month:07 https://dx.doi.org/10.1140/epja/s10050-021-00513-9 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_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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_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_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 33.40 ASE 33.50 ASE AR 57 2021 7 07 |
| allfields_unstemmed |
10.1140/epja/s10050-021-00513-9 doi (DE-627)SPR044545207 (SPR)s10050-021-00513-9-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Liu, Xingyan verfasserin aut Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021 Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neutron Source of CSNS. Two aluminum samples 70 mm in diameter and thicknesses of 40 and 60 mm, respectively, were positioned at 55 m from the neutron source. The transmission detector consisted of a multi-layer fast fission chamber loaded with %$^{235}%$U and %$^{238}%$U, and it was located at the 76-m measurement station. By applying the time-of-flight technique, it was possible to extract the n+%$^{27}%$Al total cross section in a wide energy region, from 1 eV to 20 MeV, after the correction for the double-bunch mode of the CSNS accelerator. The total cross sections obtained with the two Al samples are consistent and the results obtained with the %$^{235}%$U fission cells are in good agreement with that with %$^{238}%$U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with %$^{235}%$U for 40 mm and 60 mm thick aluminum is 0.7–22.3% and 0.6–12.4% in the energy range of 10 keV–20 MeV. Results are in fair agreement with respect to previous data and evaluations. Yang, Yiwei verfasserin aut Liu, Rong verfasserin aut Wen, Zhongwei verfasserin aut Wen, Jie verfasserin aut Han, Zijie verfasserin aut Chen, Yonghao verfasserin aut Jing, Hantao verfasserin aut Yi, Han verfasserin aut Bao, Jie verfasserin aut Ren, Zhizhou verfasserin aut An, Qi verfasserin aut Bai, Huaiyong verfasserin aut Cao, Ping verfasserin aut Chen, Qiping verfasserin aut Cheng, Pinjing verfasserin aut Cui, Zengqi verfasserin aut Fan, Ruirui verfasserin aut Feng, Changqing verfasserin aut Gu, Minhao verfasserin aut Guo, Fengqin verfasserin aut Han, Changcai verfasserin aut He, Guozhu verfasserin aut He, Yongcheng verfasserin aut He, Yuefeng verfasserin aut Huang, Hanxiong verfasserin aut Huang, Weiling verfasserin aut Huang, Xiru verfasserin aut Ji, Xiaolu verfasserin aut Ji, Xuyang verfasserin aut Jiang, Haoyu verfasserin aut Jiang, Wei verfasserin aut Kang, Ling verfasserin aut Kang, Mingtao verfasserin aut Li, Bo verfasserin aut Li, Lun verfasserin aut Li, Qiang verfasserin aut Li, Xiao verfasserin aut Li, Yang verfasserin aut Li, Yang verfasserin aut Liu, Shubin verfasserin aut Luan, Guangyuan verfasserin aut Ma, Yinglin verfasserin aut Ning, Changjun verfasserin aut Qi, Binbin verfasserin aut Ren, Jie verfasserin aut Ruan, Xichao verfasserin aut Song, Zhaohui verfasserin aut Sun, Hong verfasserin aut Sun, Xiaoyang verfasserin aut Sun, Zhijia verfasserin aut Tan, Zhixin verfasserin aut Tang, Hongqing verfasserin aut Tang, Jingyu verfasserin aut Wang, Pengcheng verfasserin aut Wang, Qi verfasserin aut Wang, Taofeng verfasserin aut Wang, Yanfeng verfasserin aut Wang, Zhaohui verfasserin aut Wang, Zheng verfasserin aut Wu, Qingbiao verfasserin aut Wu, Xiaoguang verfasserin aut Wu, Xuan verfasserin aut Xie, Likun verfasserin aut Yu, Li verfasserin aut Yu, Tao verfasserin aut Yu, Yongji verfasserin aut Zhang, Guohui verfasserin aut Zhang, Jing verfasserin aut Zhang, Linhao verfasserin aut Zhang, Liying verfasserin aut Zhang, Qingmin verfasserin aut Zhang, Qiwei verfasserin aut Zhang, Xianpeng verfasserin aut Zhang, Yuliang verfasserin aut Zhang, Zhiyong verfasserin aut Zhao, Yingtan verfasserin aut Zhou, Liang verfasserin aut Zhou, Zuying verfasserin aut Zhu, Danyang verfasserin aut Zhu, Kejun verfasserin aut Zhu, Peng verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 57(2021), 7 vom: Juli (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:57 year:2021 number:7 month:07 https://dx.doi.org/10.1140/epja/s10050-021-00513-9 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_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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_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_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 33.40 ASE 33.50 ASE AR 57 2021 7 07 |
| allfieldsGer |
10.1140/epja/s10050-021-00513-9 doi (DE-627)SPR044545207 (SPR)s10050-021-00513-9-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Liu, Xingyan verfasserin aut Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021 Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neutron Source of CSNS. Two aluminum samples 70 mm in diameter and thicknesses of 40 and 60 mm, respectively, were positioned at 55 m from the neutron source. The transmission detector consisted of a multi-layer fast fission chamber loaded with %$^{235}%$U and %$^{238}%$U, and it was located at the 76-m measurement station. By applying the time-of-flight technique, it was possible to extract the n+%$^{27}%$Al total cross section in a wide energy region, from 1 eV to 20 MeV, after the correction for the double-bunch mode of the CSNS accelerator. The total cross sections obtained with the two Al samples are consistent and the results obtained with the %$^{235}%$U fission cells are in good agreement with that with %$^{238}%$U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with %$^{235}%$U for 40 mm and 60 mm thick aluminum is 0.7–22.3% and 0.6–12.4% in the energy range of 10 keV–20 MeV. Results are in fair agreement with respect to previous data and evaluations. Yang, Yiwei verfasserin aut Liu, Rong verfasserin aut Wen, Zhongwei verfasserin aut Wen, Jie verfasserin aut Han, Zijie verfasserin aut Chen, Yonghao verfasserin aut Jing, Hantao verfasserin aut Yi, Han verfasserin aut Bao, Jie verfasserin aut Ren, Zhizhou verfasserin aut An, Qi verfasserin aut Bai, Huaiyong verfasserin aut Cao, Ping verfasserin aut Chen, Qiping verfasserin aut Cheng, Pinjing verfasserin aut Cui, Zengqi verfasserin aut Fan, Ruirui verfasserin aut Feng, Changqing verfasserin aut Gu, Minhao verfasserin aut Guo, Fengqin verfasserin aut Han, Changcai verfasserin aut He, Guozhu verfasserin aut He, Yongcheng verfasserin aut He, Yuefeng verfasserin aut Huang, Hanxiong verfasserin aut Huang, Weiling verfasserin aut Huang, Xiru verfasserin aut Ji, Xiaolu verfasserin aut Ji, Xuyang verfasserin aut Jiang, Haoyu verfasserin aut Jiang, Wei verfasserin aut Kang, Ling verfasserin aut Kang, Mingtao verfasserin aut Li, Bo verfasserin aut Li, Lun verfasserin aut Li, Qiang verfasserin aut Li, Xiao verfasserin aut Li, Yang verfasserin aut Li, Yang verfasserin aut Liu, Shubin verfasserin aut Luan, Guangyuan verfasserin aut Ma, Yinglin verfasserin aut Ning, Changjun verfasserin aut Qi, Binbin verfasserin aut Ren, Jie verfasserin aut Ruan, Xichao verfasserin aut Song, Zhaohui verfasserin aut Sun, Hong verfasserin aut Sun, Xiaoyang verfasserin aut Sun, Zhijia verfasserin aut Tan, Zhixin verfasserin aut Tang, Hongqing verfasserin aut Tang, Jingyu verfasserin aut Wang, Pengcheng verfasserin aut Wang, Qi verfasserin aut Wang, Taofeng verfasserin aut Wang, Yanfeng verfasserin aut Wang, Zhaohui verfasserin aut Wang, Zheng verfasserin aut Wu, Qingbiao verfasserin aut Wu, Xiaoguang verfasserin aut Wu, Xuan verfasserin aut Xie, Likun verfasserin aut Yu, Li verfasserin aut Yu, Tao verfasserin aut Yu, Yongji verfasserin aut Zhang, Guohui verfasserin aut Zhang, Jing verfasserin aut Zhang, Linhao verfasserin aut Zhang, Liying verfasserin aut Zhang, Qingmin verfasserin aut Zhang, Qiwei verfasserin aut Zhang, Xianpeng verfasserin aut Zhang, Yuliang verfasserin aut Zhang, Zhiyong verfasserin aut Zhao, Yingtan verfasserin aut Zhou, Liang verfasserin aut Zhou, Zuying verfasserin aut Zhu, Danyang verfasserin aut Zhu, Kejun verfasserin aut Zhu, Peng verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 57(2021), 7 vom: Juli (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:57 year:2021 number:7 month:07 https://dx.doi.org/10.1140/epja/s10050-021-00513-9 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_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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_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_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 33.40 ASE 33.50 ASE AR 57 2021 7 07 |
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10.1140/epja/s10050-021-00513-9 doi (DE-627)SPR044545207 (SPR)s10050-021-00513-9-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Liu, Xingyan verfasserin aut Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021 Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neutron Source of CSNS. Two aluminum samples 70 mm in diameter and thicknesses of 40 and 60 mm, respectively, were positioned at 55 m from the neutron source. The transmission detector consisted of a multi-layer fast fission chamber loaded with %$^{235}%$U and %$^{238}%$U, and it was located at the 76-m measurement station. By applying the time-of-flight technique, it was possible to extract the n+%$^{27}%$Al total cross section in a wide energy region, from 1 eV to 20 MeV, after the correction for the double-bunch mode of the CSNS accelerator. The total cross sections obtained with the two Al samples are consistent and the results obtained with the %$^{235}%$U fission cells are in good agreement with that with %$^{238}%$U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with %$^{235}%$U for 40 mm and 60 mm thick aluminum is 0.7–22.3% and 0.6–12.4% in the energy range of 10 keV–20 MeV. Results are in fair agreement with respect to previous data and evaluations. Yang, Yiwei verfasserin aut Liu, Rong verfasserin aut Wen, Zhongwei verfasserin aut Wen, Jie verfasserin aut Han, Zijie verfasserin aut Chen, Yonghao verfasserin aut Jing, Hantao verfasserin aut Yi, Han verfasserin aut Bao, Jie verfasserin aut Ren, Zhizhou verfasserin aut An, Qi verfasserin aut Bai, Huaiyong verfasserin aut Cao, Ping verfasserin aut Chen, Qiping verfasserin aut Cheng, Pinjing verfasserin aut Cui, Zengqi verfasserin aut Fan, Ruirui verfasserin aut Feng, Changqing verfasserin aut Gu, Minhao verfasserin aut Guo, Fengqin verfasserin aut Han, Changcai verfasserin aut He, Guozhu verfasserin aut He, Yongcheng verfasserin aut He, Yuefeng verfasserin aut Huang, Hanxiong verfasserin aut Huang, Weiling verfasserin aut Huang, Xiru verfasserin aut Ji, Xiaolu verfasserin aut Ji, Xuyang verfasserin aut Jiang, Haoyu verfasserin aut Jiang, Wei verfasserin aut Kang, Ling verfasserin aut Kang, Mingtao verfasserin aut Li, Bo verfasserin aut Li, Lun verfasserin aut Li, Qiang verfasserin aut Li, Xiao verfasserin aut Li, Yang verfasserin aut Li, Yang verfasserin aut Liu, Shubin verfasserin aut Luan, Guangyuan verfasserin aut Ma, Yinglin verfasserin aut Ning, Changjun verfasserin aut Qi, Binbin verfasserin aut Ren, Jie verfasserin aut Ruan, Xichao verfasserin aut Song, Zhaohui verfasserin aut Sun, Hong verfasserin aut Sun, Xiaoyang verfasserin aut Sun, Zhijia verfasserin aut Tan, Zhixin verfasserin aut Tang, Hongqing verfasserin aut Tang, Jingyu verfasserin aut Wang, Pengcheng verfasserin aut Wang, Qi verfasserin aut Wang, Taofeng verfasserin aut Wang, Yanfeng verfasserin aut Wang, Zhaohui verfasserin aut Wang, Zheng verfasserin aut Wu, Qingbiao verfasserin aut Wu, Xiaoguang verfasserin aut Wu, Xuan verfasserin aut Xie, Likun verfasserin aut Yu, Li verfasserin aut Yu, Tao verfasserin aut Yu, Yongji verfasserin aut Zhang, Guohui verfasserin aut Zhang, Jing verfasserin aut Zhang, Linhao verfasserin aut Zhang, Liying verfasserin aut Zhang, Qingmin verfasserin aut Zhang, Qiwei verfasserin aut Zhang, Xianpeng verfasserin aut Zhang, Yuliang verfasserin aut Zhang, Zhiyong verfasserin aut Zhao, Yingtan verfasserin aut Zhou, Liang verfasserin aut Zhou, Zuying verfasserin aut Zhu, Danyang verfasserin aut Zhu, Kejun verfasserin aut Zhu, Peng verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 57(2021), 7 vom: Juli (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:57 year:2021 number:7 month:07 https://dx.doi.org/10.1140/epja/s10050-021-00513-9 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_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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 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_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_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 33.40 ASE 33.50 ASE AR 57 2021 7 07 |
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530 ASE 33.40 bkl 33.50 bkl Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS |
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Liu, Xingyan Yang, Yiwei Liu, Rong Wen, Zhongwei Wen, Jie Han, Zijie Chen, Yonghao Jing, Hantao Yi, Han Bao, Jie Ren, Zhizhou An, Qi Bai, Huaiyong Cao, Ping Chen, Qiping Cheng, Pinjing Cui, Zengqi Fan, Ruirui Feng, Changqing Gu, Minhao Guo, Fengqin Han, Changcai He, Guozhu He, Yongcheng He, Yuefeng Huang, Hanxiong Huang, Weiling Huang, Xiru Ji, Xiaolu Ji, Xuyang Jiang, Haoyu Jiang, Wei Kang, Ling Kang, Mingtao Li, Bo Li, Lun Li, Qiang Li, Xiao Li, Yang Liu, Shubin Luan, Guangyuan Ma, Yinglin Ning, Changjun Qi, Binbin Ren, Jie Ruan, Xichao 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 Wu, Qingbiao Wu, Xiaoguang Wu, Xuan Xie, Likun 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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measurement of the neutron total cross sections of aluminum at the back-n white neutron source of csns |
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Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS |
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Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neutron Source of CSNS. Two aluminum samples 70 mm in diameter and thicknesses of 40 and 60 mm, respectively, were positioned at 55 m from the neutron source. The transmission detector consisted of a multi-layer fast fission chamber loaded with %$^{235}%$U and %$^{238}%$U, and it was located at the 76-m measurement station. By applying the time-of-flight technique, it was possible to extract the n+%$^{27}%$Al total cross section in a wide energy region, from 1 eV to 20 MeV, after the correction for the double-bunch mode of the CSNS accelerator. The total cross sections obtained with the two Al samples are consistent and the results obtained with the %$^{235}%$U fission cells are in good agreement with that with %$^{238}%$U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with %$^{235}%$U for 40 mm and 60 mm thick aluminum is 0.7–22.3% and 0.6–12.4% in the energy range of 10 keV–20 MeV. Results are in fair agreement with respect to previous data and evaluations. © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021 |
| abstractGer |
Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neutron Source of CSNS. Two aluminum samples 70 mm in diameter and thicknesses of 40 and 60 mm, respectively, were positioned at 55 m from the neutron source. The transmission detector consisted of a multi-layer fast fission chamber loaded with %$^{235}%$U and %$^{238}%$U, and it was located at the 76-m measurement station. By applying the time-of-flight technique, it was possible to extract the n+%$^{27}%$Al total cross section in a wide energy region, from 1 eV to 20 MeV, after the correction for the double-bunch mode of the CSNS accelerator. The total cross sections obtained with the two Al samples are consistent and the results obtained with the %$^{235}%$U fission cells are in good agreement with that with %$^{238}%$U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with %$^{235}%$U for 40 mm and 60 mm thick aluminum is 0.7–22.3% and 0.6–12.4% in the energy range of 10 keV–20 MeV. Results are in fair agreement with respect to previous data and evaluations. © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021 |
| abstract_unstemmed |
Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neutron Source of CSNS. Two aluminum samples 70 mm in diameter and thicknesses of 40 and 60 mm, respectively, were positioned at 55 m from the neutron source. The transmission detector consisted of a multi-layer fast fission chamber loaded with %$^{235}%$U and %$^{238}%$U, and it was located at the 76-m measurement station. By applying the time-of-flight technique, it was possible to extract the n+%$^{27}%$Al total cross section in a wide energy region, from 1 eV to 20 MeV, after the correction for the double-bunch mode of the CSNS accelerator. The total cross sections obtained with the two Al samples are consistent and the results obtained with the %$^{235}%$U fission cells are in good agreement with that with %$^{238}%$U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with %$^{235}%$U for 40 mm and 60 mm thick aluminum is 0.7–22.3% and 0.6–12.4% in the energy range of 10 keV–20 MeV. Results are in fair agreement with respect to previous data and evaluations. © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021 |
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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">SPR044545207</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220110201545.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">210715s2021 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1140/epja/s10050-021-00513-9</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR044545207</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10050-021-00513-9-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="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.40</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.50</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Liu, Xingyan</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS</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">© The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2021. corrected publication 2021</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Aluminum and its alloys are widely used in the nuclear industry. Therefore, it is essential to precisely measure and accurately know the neutron total cross section of aluminum in the wider energy region. The measurement is performed by using the transmission method at the Back-n White Neutron Source of CSNS. Two aluminum samples 70 mm in diameter and thicknesses of 40 and 60 mm, respectively, were positioned at 55 m from the neutron source. The transmission detector consisted of a multi-layer fast fission chamber loaded with %$^{235}%$U and %$^{238}%$U, and it was located at the 76-m measurement station. By applying the time-of-flight technique, it was possible to extract the n+%$^{27}%$Al total cross section in a wide energy region, from 1 eV to 20 MeV, after the correction for the double-bunch mode of the CSNS accelerator. The total cross sections obtained with the two Al samples are consistent and the results obtained with the %$^{235}%$U fission cells are in good agreement with that with %$^{238}%$U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with %$^{235}%$U for 40 mm and 60 mm thick aluminum is 0.7–22.3% and 0.6–12.4% in the energy range of 10 keV–20 MeV. 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| score |
7.401026 |