Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS

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作者
Xingyan Liu
Yiwei Yang
Rong Liu
Zhongwei Wen
Jie Wen
Zijie Han
Yonghao Chen
Hantao Jing
Han Yi
Jie Bao
Zhizhou Ren
Qi An
Huaiyong Bai
Ping Cao
Qiping Chen
Pinjing Cheng
Zengqi Cui
Ruirui Fan
Changqing Feng
Minhao Gu
Fengqin Guo
Changcai Han
Guozhu He
Yongcheng He
Yuefeng He
Hanxiong Huang
Weiling Huang
Xiru Huang
Xiaolu Ji
Xuyang Ji
Haoyu Jiang
Wei Jiang
Ling Kang
Mingtao Kang
Bo Li
Lun Li
Qiang Li
Xiao Li
Yang Li
Yang Li
Shubin Liu
Guangyuan Luan
Yinglin Ma
Changjun Ning
Binbin Qi
Jie Ren
Xichao Ruan
Zhaohui Song
Hong Sun
Xiaoyang Sun
机构
[1] China Academy of Engineering Physics,Institute of Nuclear Physics and Chemistry
[2] Chinese Academy of Sciences (CAS),Institute of High Energy Physics
[3] Spallation Neutron Source Science Center,Key Laboratory of Nuclear Data
[4] China Institute of Atomic Energy,Department of Modern Physics
[5] State Key Laboratory of Particle Detection and Electronics,State Key Laboratory of Nuclear Physics and Technology, School of Physics
[6] University of Science and Technology of China,Department of Engineering and Applied Physics
[7] Peking University,School of Physics
[8] University of South China,undefined
[9] Northwest Institute of Nuclear Technology,undefined
[10] University of Science and Technology of China,undefined
[11] Beihang University,undefined
[12] Xi’an Jiaotong University,undefined
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摘要
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\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{235}$$\end{document}U and 238\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{238}$$\end{document}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\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{27}$$\end{document}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\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{235}$$\end{document}U fission cells are in good agreement with that with 238\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{238}$$\end{document}U in the energy range of 1–20 MeV. The uncertainty of neutron total cross section measured with 235\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{235}$$\end{document}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.
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