TY - JOUR
T1 - Neutron energy spectrum measurement using an NE213 scintillator at CHARM
AU - Kajimoto, Tsuyoshi
AU - Sanami, Toshiya
AU - Nakao, Noriaki
AU - Froeschl, Robert
AU - Roesler, Stefan
AU - Iliopoulou, Elpida
AU - Infantino, Angelo
AU - Brugger, Markus
AU - Lee, Eunji
AU - Shigyo, Nobuhiro
AU - Hagiwara, Masayuki
AU - Yashima, Hiroshi
AU - Yamazaki, Hirohito
AU - Tanaka, Kenichi
AU - Endo, Satoru
N1 - Publisher Copyright:
© 2018 Elsevier B.V.
PY - 2018/8/15
Y1 - 2018/8/15
N2 - To establish a methodology for neutron spectrum measurement at the CERN High energy AcceleRator Mixed field facility (CHARM), neutron spectra were measured using an NE213 scintillator on top of the CHARM roof shielding where is the CERN Shielding Benchmark Facility (CSBF). The spectra were derived as fluences into the scintillator by the unfolding method using an iterative Bayesian algorithm. The methodology was verified based on the agreement of two spectra measured for different positions and directions of incident neutrons by changing the detector orientation. Since the spectra on the roof-top were obtained within a reasonable beam-time, this methodology is suitable for measuring the spectrum when there is less shielding material. Thus, experimental data for neutron transition can be obtained as a function of shielding thickness using this facility.
AB - To establish a methodology for neutron spectrum measurement at the CERN High energy AcceleRator Mixed field facility (CHARM), neutron spectra were measured using an NE213 scintillator on top of the CHARM roof shielding where is the CERN Shielding Benchmark Facility (CSBF). The spectra were derived as fluences into the scintillator by the unfolding method using an iterative Bayesian algorithm. The methodology was verified based on the agreement of two spectra measured for different positions and directions of incident neutrons by changing the detector orientation. Since the spectra on the roof-top were obtained within a reasonable beam-time, this methodology is suitable for measuring the spectrum when there is less shielding material. Thus, experimental data for neutron transition can be obtained as a function of shielding thickness using this facility.
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U2 - 10.1016/j.nimb.2018.05.024
DO - 10.1016/j.nimb.2018.05.024
M3 - Article
AN - SCOPUS:85047375995
SN - 0168-583X
VL - 429
SP - 27
EP - 33
JO - Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
JF - Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
ER -