Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n
Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections r...
Ausführliche Beschreibung
Autor*in: |
Ren, Zhizhou [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2023 |
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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 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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Übergeordnetes Werk: |
Enthalten in: The European physical journal - Berlin : Springer, 1998, 59(2023), 1 vom: 13. Jan. |
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Übergeordnetes Werk: |
volume:59 ; year:2023 ; number:1 ; day:13 ; month:01 |
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DOI / URN: |
10.1140/epja/s10050-022-00910-8 |
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Katalog-ID: |
SPR049470426 |
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520 | |a Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections relative to 235U from the threshold to 200 MeV was carried out by using time-of-flight (TOF) method with a multi-cell fast fission ionization chamber in double-bunch mode. The TOF spectra in double-bunch mode were unfolded by using Bayesian method. The fission cross section ratios of 238U/235U and 236U/235U were obtained. The experimental data of the 236,238U/235U fission cross section ratios measured in single-bunch mode were re-analyzed in high energy region and the upper limit was extended to 200 MeV for comparison. The experimental results in double-bunch mode are in good agreement with those in single-bunch mode and the main evaluation data within experimental uncertainties. The 236,238U(n,f) cross sections were obtained from the measured ratios and the standard 235U(n,f) cross sections and they agree well with the theoretical calculation, previous experiments, main evaluations and IAEA NDS. The experimental results can provide technical support for further experimental researches in double-bunch mode and relevant nuclear data evaluations. | ||
700 | 1 | |a Yang, Yiwei |4 aut | |
700 | 1 | |a Liu, Rong |4 aut | |
700 | 1 | |a Ye, Bangjiao |4 aut | |
700 | 1 | |a Wen, Zhongwei |4 aut | |
700 | 1 | |a Wen, Jie |4 aut | |
700 | 1 | |a Guo, Hairui |4 aut | |
700 | 1 | |a Chen, Yonghao |4 aut | |
700 | 1 | |a Yi, Han |4 aut | |
700 | 1 | |a Sun, Weili |4 aut | |
700 | 1 | |a Yan, Jie |4 aut | |
700 | 1 | |a Han, Zijie |4 aut | |
700 | 1 | |a Liu, Xingyan |4 aut | |
700 | 1 | |a Chen, Qiping |4 aut | |
700 | 1 | |a Ye, Tao |4 aut | |
700 | 1 | |a Bai, Jiangbo |4 aut | |
700 | 1 | |a An, Qi |4 aut | |
700 | 1 | |a Bai, Huaiyong |4 aut | |
700 | 1 | |a Bao, Jie |4 aut | |
700 | 1 | |a Cao, Ping |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 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 Jiang, Wei |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, Shubin |4 aut | |
700 | 1 | |a Luan, Guangyuan |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 Ren, Jie |4 aut | |
700 | 1 | |a Ruan, Xichao |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 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 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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10.1140/epja/s10050-022-00910-8 doi (DE-627)SPR049470426 (SPR)s10050-022-00910-8-e DE-627 ger DE-627 rakwb eng Ren, Zhizhou verfasserin (orcid)0000-0002-6524-6357 aut Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n 2023 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 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections relative to 235U from the threshold to 200 MeV was carried out by using time-of-flight (TOF) method with a multi-cell fast fission ionization chamber in double-bunch mode. The TOF spectra in double-bunch mode were unfolded by using Bayesian method. The fission cross section ratios of 238U/235U and 236U/235U were obtained. The experimental data of the 236,238U/235U fission cross section ratios measured in single-bunch mode were re-analyzed in high energy region and the upper limit was extended to 200 MeV for comparison. The experimental results in double-bunch mode are in good agreement with those in single-bunch mode and the main evaluation data within experimental uncertainties. The 236,238U(n,f) cross sections were obtained from the measured ratios and the standard 235U(n,f) cross sections and they agree well with the theoretical calculation, previous experiments, main evaluations and IAEA NDS. The experimental results can provide technical support for further experimental researches in double-bunch mode and relevant nuclear data evaluations. Yang, Yiwei aut Liu, Rong aut Ye, Bangjiao aut Wen, Zhongwei aut Wen, Jie aut Guo, Hairui aut Chen, Yonghao aut Yi, Han aut Sun, Weili aut Yan, Jie aut Han, Zijie aut Liu, Xingyan aut Chen, Qiping aut Ye, Tao aut Bai, Jiangbo aut An, Qi aut Bai, Huaiyong aut Bao, Jie aut Cao, Ping aut Cheng, Pinjing aut Cui, Zengqi aut Fan, Ruirui aut Feng, Changqing aut Gu, Minhao aut Guo, Fengqin aut Han, Changcai 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 Jiang, Wei 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, Shubin aut Luan, Guangyuan aut Ma, Yinglin aut Ning, Changjun aut Qi, Binbin aut Ren, Jie aut Ruan, Xichao 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 Wu, Qingbiao aut Wu, Xiaoguang aut Wu, Xuan aut Xie, Likun 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 The European physical journal Berlin : Springer, 1998 59(2023), 1 vom: 13. Jan. (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:59 year:2023 number:1 day:13 month:01 https://dx.doi.org/10.1140/epja/s10050-022-00910-8 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_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 AR 59 2023 1 13 01 |
spelling |
10.1140/epja/s10050-022-00910-8 doi (DE-627)SPR049470426 (SPR)s10050-022-00910-8-e DE-627 ger DE-627 rakwb eng Ren, Zhizhou verfasserin (orcid)0000-0002-6524-6357 aut Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n 2023 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 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections relative to 235U from the threshold to 200 MeV was carried out by using time-of-flight (TOF) method with a multi-cell fast fission ionization chamber in double-bunch mode. The TOF spectra in double-bunch mode were unfolded by using Bayesian method. The fission cross section ratios of 238U/235U and 236U/235U were obtained. The experimental data of the 236,238U/235U fission cross section ratios measured in single-bunch mode were re-analyzed in high energy region and the upper limit was extended to 200 MeV for comparison. The experimental results in double-bunch mode are in good agreement with those in single-bunch mode and the main evaluation data within experimental uncertainties. The 236,238U(n,f) cross sections were obtained from the measured ratios and the standard 235U(n,f) cross sections and they agree well with the theoretical calculation, previous experiments, main evaluations and IAEA NDS. The experimental results can provide technical support for further experimental researches in double-bunch mode and relevant nuclear data evaluations. Yang, Yiwei aut Liu, Rong aut Ye, Bangjiao aut Wen, Zhongwei aut Wen, Jie aut Guo, Hairui aut Chen, Yonghao aut Yi, Han aut Sun, Weili aut Yan, Jie aut Han, Zijie aut Liu, Xingyan aut Chen, Qiping aut Ye, Tao aut Bai, Jiangbo aut An, Qi aut Bai, Huaiyong aut Bao, Jie aut Cao, Ping aut Cheng, Pinjing aut Cui, Zengqi aut Fan, Ruirui aut Feng, Changqing aut Gu, Minhao aut Guo, Fengqin aut Han, Changcai 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 Jiang, Wei 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, Shubin aut Luan, Guangyuan aut Ma, Yinglin aut Ning, Changjun aut Qi, Binbin aut Ren, Jie aut Ruan, Xichao 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 Wu, Qingbiao aut Wu, Xiaoguang aut Wu, Xuan aut Xie, Likun 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 The European physical journal Berlin : Springer, 1998 59(2023), 1 vom: 13. Jan. (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:59 year:2023 number:1 day:13 month:01 https://dx.doi.org/10.1140/epja/s10050-022-00910-8 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_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 AR 59 2023 1 13 01 |
allfields_unstemmed |
10.1140/epja/s10050-022-00910-8 doi (DE-627)SPR049470426 (SPR)s10050-022-00910-8-e DE-627 ger DE-627 rakwb eng Ren, Zhizhou verfasserin (orcid)0000-0002-6524-6357 aut Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n 2023 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 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections relative to 235U from the threshold to 200 MeV was carried out by using time-of-flight (TOF) method with a multi-cell fast fission ionization chamber in double-bunch mode. The TOF spectra in double-bunch mode were unfolded by using Bayesian method. The fission cross section ratios of 238U/235U and 236U/235U were obtained. The experimental data of the 236,238U/235U fission cross section ratios measured in single-bunch mode were re-analyzed in high energy region and the upper limit was extended to 200 MeV for comparison. The experimental results in double-bunch mode are in good agreement with those in single-bunch mode and the main evaluation data within experimental uncertainties. The 236,238U(n,f) cross sections were obtained from the measured ratios and the standard 235U(n,f) cross sections and they agree well with the theoretical calculation, previous experiments, main evaluations and IAEA NDS. The experimental results can provide technical support for further experimental researches in double-bunch mode and relevant nuclear data evaluations. Yang, Yiwei aut Liu, Rong aut Ye, Bangjiao aut Wen, Zhongwei aut Wen, Jie aut Guo, Hairui aut Chen, Yonghao aut Yi, Han aut Sun, Weili aut Yan, Jie aut Han, Zijie aut Liu, Xingyan aut Chen, Qiping aut Ye, Tao aut Bai, Jiangbo aut An, Qi aut Bai, Huaiyong aut Bao, Jie aut Cao, Ping aut Cheng, Pinjing aut Cui, Zengqi aut Fan, Ruirui aut Feng, Changqing aut Gu, Minhao aut Guo, Fengqin aut Han, Changcai 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 Jiang, Wei 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, Shubin aut Luan, Guangyuan aut Ma, Yinglin aut Ning, Changjun aut Qi, Binbin aut Ren, Jie aut Ruan, Xichao 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 Wu, Qingbiao aut Wu, Xiaoguang aut Wu, Xuan aut Xie, Likun 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 The European physical journal Berlin : Springer, 1998 59(2023), 1 vom: 13. Jan. (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:59 year:2023 number:1 day:13 month:01 https://dx.doi.org/10.1140/epja/s10050-022-00910-8 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_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 AR 59 2023 1 13 01 |
allfieldsGer |
10.1140/epja/s10050-022-00910-8 doi (DE-627)SPR049470426 (SPR)s10050-022-00910-8-e DE-627 ger DE-627 rakwb eng Ren, Zhizhou verfasserin (orcid)0000-0002-6524-6357 aut Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n 2023 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 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections relative to 235U from the threshold to 200 MeV was carried out by using time-of-flight (TOF) method with a multi-cell fast fission ionization chamber in double-bunch mode. The TOF spectra in double-bunch mode were unfolded by using Bayesian method. The fission cross section ratios of 238U/235U and 236U/235U were obtained. The experimental data of the 236,238U/235U fission cross section ratios measured in single-bunch mode were re-analyzed in high energy region and the upper limit was extended to 200 MeV for comparison. The experimental results in double-bunch mode are in good agreement with those in single-bunch mode and the main evaluation data within experimental uncertainties. The 236,238U(n,f) cross sections were obtained from the measured ratios and the standard 235U(n,f) cross sections and they agree well with the theoretical calculation, previous experiments, main evaluations and IAEA NDS. The experimental results can provide technical support for further experimental researches in double-bunch mode and relevant nuclear data evaluations. Yang, Yiwei aut Liu, Rong aut Ye, Bangjiao aut Wen, Zhongwei aut Wen, Jie aut Guo, Hairui aut Chen, Yonghao aut Yi, Han aut Sun, Weili aut Yan, Jie aut Han, Zijie aut Liu, Xingyan aut Chen, Qiping aut Ye, Tao aut Bai, Jiangbo aut An, Qi aut Bai, Huaiyong aut Bao, Jie aut Cao, Ping aut Cheng, Pinjing aut Cui, Zengqi aut Fan, Ruirui aut Feng, Changqing aut Gu, Minhao aut Guo, Fengqin aut Han, Changcai 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 Jiang, Wei 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, Shubin aut Luan, Guangyuan aut Ma, Yinglin aut Ning, Changjun aut Qi, Binbin aut Ren, Jie aut Ruan, Xichao 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 Wu, Qingbiao aut Wu, Xiaoguang aut Wu, Xuan aut Xie, Likun 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 The European physical journal Berlin : Springer, 1998 59(2023), 1 vom: 13. Jan. (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:59 year:2023 number:1 day:13 month:01 https://dx.doi.org/10.1140/epja/s10050-022-00910-8 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_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 AR 59 2023 1 13 01 |
allfieldsSound |
10.1140/epja/s10050-022-00910-8 doi (DE-627)SPR049470426 (SPR)s10050-022-00910-8-e DE-627 ger DE-627 rakwb eng Ren, Zhizhou verfasserin (orcid)0000-0002-6524-6357 aut Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n 2023 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 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections relative to 235U from the threshold to 200 MeV was carried out by using time-of-flight (TOF) method with a multi-cell fast fission ionization chamber in double-bunch mode. The TOF spectra in double-bunch mode were unfolded by using Bayesian method. The fission cross section ratios of 238U/235U and 236U/235U were obtained. The experimental data of the 236,238U/235U fission cross section ratios measured in single-bunch mode were re-analyzed in high energy region and the upper limit was extended to 200 MeV for comparison. The experimental results in double-bunch mode are in good agreement with those in single-bunch mode and the main evaluation data within experimental uncertainties. The 236,238U(n,f) cross sections were obtained from the measured ratios and the standard 235U(n,f) cross sections and they agree well with the theoretical calculation, previous experiments, main evaluations and IAEA NDS. The experimental results can provide technical support for further experimental researches in double-bunch mode and relevant nuclear data evaluations. Yang, Yiwei aut Liu, Rong aut Ye, Bangjiao aut Wen, Zhongwei aut Wen, Jie aut Guo, Hairui aut Chen, Yonghao aut Yi, Han aut Sun, Weili aut Yan, Jie aut Han, Zijie aut Liu, Xingyan aut Chen, Qiping aut Ye, Tao aut Bai, Jiangbo aut An, Qi aut Bai, Huaiyong aut Bao, Jie aut Cao, Ping aut Cheng, Pinjing aut Cui, Zengqi aut Fan, Ruirui aut Feng, Changqing aut Gu, Minhao aut Guo, Fengqin aut Han, Changcai 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 Jiang, Wei 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, Shubin aut Luan, Guangyuan aut Ma, Yinglin aut Ning, Changjun aut Qi, Binbin aut Ren, Jie aut Ruan, Xichao 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 Wu, Qingbiao aut Wu, Xiaoguang aut Wu, Xuan aut Xie, Likun 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 The European physical journal Berlin : Springer, 1998 59(2023), 1 vom: 13. Jan. 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Enthalten in The European physical journal 59(2023), 1 vom: 13. Jan. volume:59 year:2023 number:1 day:13 month:01 |
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Ren, Zhizhou @@aut@@ Yang, Yiwei @@aut@@ Liu, Rong @@aut@@ Ye, Bangjiao @@aut@@ Wen, Zhongwei @@aut@@ Wen, Jie @@aut@@ Guo, Hairui @@aut@@ Chen, Yonghao @@aut@@ Yi, Han @@aut@@ Sun, Weili @@aut@@ Yan, Jie @@aut@@ Han, Zijie @@aut@@ Liu, Xingyan @@aut@@ Chen, Qiping @@aut@@ Ye, Tao @@aut@@ Bai, Jiangbo @@aut@@ An, Qi @@aut@@ Bai, Huaiyong @@aut@@ Bao, Jie @@aut@@ Cao, Ping @@aut@@ Cheng, Pinjing @@aut@@ Cui, Zengqi @@aut@@ Fan, Ruirui @@aut@@ Feng, Changqing @@aut@@ Gu, Minhao @@aut@@ Guo, Fengqin @@aut@@ Han, Changcai @@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@@ Jiang, Wei @@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, Shubin @@aut@@ Luan, Guangyuan @@aut@@ Ma, Yinglin @@aut@@ Ning, Changjun @@aut@@ Qi, Binbin @@aut@@ Ren, Jie @@aut@@ Ruan, Xichao @@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@@ Wu, Qingbiao @@aut@@ Wu, Xiaoguang @@aut@@ Wu, Xuan @@aut@@ Xie, Likun @@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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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000naa a22002652 4500</leader><controlfield tag="001">SPR049470426</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230227064601.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230227s2023 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1140/epja/s10050-022-00910-8</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR049470426</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10050-022-00910-8-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, Zhizhou</subfield><subfield code="e">verfasserin</subfield><subfield code="0">(orcid)0000-0002-6524-6357</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2023</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 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections relative to 235U from the threshold to 200 MeV was carried out by using time-of-flight (TOF) method with a multi-cell fast fission ionization chamber in double-bunch mode. The TOF spectra in double-bunch mode were unfolded by using Bayesian method. The fission cross section ratios of 238U/235U and 236U/235U were obtained. The experimental data of the 236,238U/235U fission cross section ratios measured in single-bunch mode were re-analyzed in high energy region and the upper limit was extended to 200 MeV for comparison. The experimental results in double-bunch mode are in good agreement with those in single-bunch mode and the main evaluation data within experimental uncertainties. The 236,238U(n,f) cross sections were obtained from the measured ratios and the standard 235U(n,f) cross sections and they agree well with the theoretical calculation, previous experiments, main evaluations and IAEA NDS. 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Ren, Zhizhou |
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Ren, Zhizhou Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n |
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Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n |
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Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n |
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Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n |
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Ren, Zhizhou Yang, Yiwei Liu, Rong Ye, Bangjiao Wen, Zhongwei Wen, Jie Guo, Hairui Chen, Yonghao Yi, Han Sun, Weili Yan, Jie Han, Zijie Liu, Xingyan Chen, Qiping Ye, Tao Bai, Jiangbo An, Qi Bai, Huaiyong Bao, Jie Cao, Ping 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 Jing, Hantao 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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Ren, Zhizhou |
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10.1140/epja/s10050-022-00910-8 |
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measurement of the 236,238u(n,f) cross sections from the threshold to 200 mev at csns back-n |
title_auth |
Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n |
abstract |
Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections relative to 235U from the threshold to 200 MeV was carried out by using time-of-flight (TOF) method with a multi-cell fast fission ionization chamber in double-bunch mode. The TOF spectra in double-bunch mode were unfolded by using Bayesian method. The fission cross section ratios of 238U/235U and 236U/235U were obtained. The experimental data of the 236,238U/235U fission cross section ratios measured in single-bunch mode were re-analyzed in high energy region and the upper limit was extended to 200 MeV for comparison. The experimental results in double-bunch mode are in good agreement with those in single-bunch mode and the main evaluation data within experimental uncertainties. The 236,238U(n,f) cross sections were obtained from the measured ratios and the standard 235U(n,f) cross sections and they agree well with the theoretical calculation, previous experiments, main evaluations and IAEA NDS. The experimental results can provide technical support for further experimental researches in double-bunch mode and relevant nuclear data evaluations. © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
abstractGer |
Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections relative to 235U from the threshold to 200 MeV was carried out by using time-of-flight (TOF) method with a multi-cell fast fission ionization chamber in double-bunch mode. The TOF spectra in double-bunch mode were unfolded by using Bayesian method. The fission cross section ratios of 238U/235U and 236U/235U were obtained. The experimental data of the 236,238U/235U fission cross section ratios measured in single-bunch mode were re-analyzed in high energy region and the upper limit was extended to 200 MeV for comparison. The experimental results in double-bunch mode are in good agreement with those in single-bunch mode and the main evaluation data within experimental uncertainties. The 236,238U(n,f) cross sections were obtained from the measured ratios and the standard 235U(n,f) cross sections and they agree well with the theoretical calculation, previous experiments, main evaluations and IAEA NDS. The experimental results can provide technical support for further experimental researches in double-bunch mode and relevant nuclear data evaluations. © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
abstract_unstemmed |
Abstract Neutron-induced uranium fission reactions play an essential role in advanced nuclear energy research, basic and applied nuclear science. Based on the China Spallation Neutron Source (CSNS) Back-streaming white neutron source (Back-n), the measurement of the 236,238U fission cross sections relative to 235U from the threshold to 200 MeV was carried out by using time-of-flight (TOF) method with a multi-cell fast fission ionization chamber in double-bunch mode. The TOF spectra in double-bunch mode were unfolded by using Bayesian method. The fission cross section ratios of 238U/235U and 236U/235U were obtained. The experimental data of the 236,238U/235U fission cross section ratios measured in single-bunch mode were re-analyzed in high energy region and the upper limit was extended to 200 MeV for comparison. The experimental results in double-bunch mode are in good agreement with those in single-bunch mode and the main evaluation data within experimental uncertainties. The 236,238U(n,f) cross sections were obtained from the measured ratios and the standard 235U(n,f) cross sections and they agree well with the theoretical calculation, previous experiments, main evaluations and IAEA NDS. The experimental results can provide technical support for further experimental researches in double-bunch mode and relevant nuclear data evaluations. © The Author(s), under exclusive licence to Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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Measurement of the 236,238U(n,f) cross sections from the threshold to 200 MeV at CSNS Back-n |
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Yang, Yiwei Liu, Rong Ye, Bangjiao Wen, Zhongwei Wen, Jie Guo, Hairui Chen, Yonghao Yi, Han Sun, Weili Yan, Jie Han, Zijie Liu, Xingyan Chen, Qiping Ye, Tao Bai, Jiangbo An, Qi Bai, Huaiyong Bao, Jie Cao, Ping 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 Jing, Hantao 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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Yang, Yiwei Liu, Rong Ye, Bangjiao Wen, Zhongwei Wen, Jie Guo, Hairui Chen, Yonghao Yi, Han Sun, Weili Yan, Jie Han, Zijie Liu, Xingyan Chen, Qiping Ye, Tao Bai, Jiangbo An, Qi Bai, Huaiyong Bao, Jie Cao, Ping 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 Jing, Hantao 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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