scholarly journals Neutron production from thick LiF, C, Si, Ni, Mo, and Ta targets bombarded by 13.4-MeV deuterons

2020 ◽  
Vol 239 ◽  
pp. 01018
Author(s):  
Hayato Takeshita ◽  
Yukinobu Watanabe ◽  
Keita Nakano ◽  
Seiya Manabe ◽  
Katsumi Aoki ◽  
...  

Double-differential thick target neutron yields from LiF, C, Si, Ni, Mo, and Ta targets bombarded by 13.4-MeV deuterons were measured by using an EJ-301 liquid organic scintillator at the Center for Accelerator and Beam Applied Science, Kyushu University. The measured (d, xn) spectra were compared with the (t, xn) spectra measured by the other group at the same incident energy per nucleon (6.7 MeV/u) and theoretical model calculations by Particle and Heavy Ion Transport code System (PHITS) and DEUteron-induced Reaction Analysis Code System (DEURACS). Some bumps are observed in the (d, xn) spectra for low-Z target elements, while no specific structure was seen in the (t, xn) spectra. The PHITS calculation, in which the intra-nuclear cascade of Liége (INCL) and generalized evaporation model (GEM) were used, generally overestimates neutron spectra while the DEURACS calculation agrees with experimental ones fairly well.

2020 ◽  
Vol 239 ◽  
pp. 20006
Author(s):  
Keita Nakano ◽  
Yukinobu Watanabe ◽  
Shoichiro Kawase ◽  
He Wang ◽  
Hideaki Otsu ◽  
...  

The isotope-production cross sections in p- and d-induced reactions on 93Zr at approximately 50 MeV/nucleon were measured by using the inverse-kinematics method at RIKEN RI Beam Factory. The measured data were compared with the previous experimental 93Zr + p, d at 105 and 209 MeV/nucleon data. This comparison represents that the isotopic distribution of production cross sections at 51 MeV p-induced reaction is appreciably different from those at 105 and 209 MeV. On the other hand, these three data sets show that the shape of isotopic distribution is similar in the case of the d-induced reaction. Also, the measured production cross sections were compared with the theoretical model calculations with Particle and Heavy Ion Transport code System (PHITS) version 3.10 in order to investigate the reproducibility of the models implemented in PHITS. The calculations well reproduced the experimental data even in such low incident energy, while several discrepancies were still seen as in the p- and d-induced reactions at 105 and 209 MeV/nucleon.


Author(s):  
Tatsuhiko Sato ◽  
Koji Niita ◽  
Norihiro Matsuda ◽  
Shintaro Hashimoto ◽  
Yosuke Iwamoto ◽  
...  

2007 ◽  
Vol 46 (6A) ◽  
pp. 3377-3379
Author(s):  
Yutaka Arita ◽  
Koji Niita ◽  
Yuji Kihara ◽  
Junich Mitsuhasi ◽  
Mikio Takai ◽  
...  

2011 ◽  
Vol 59 (2(3)) ◽  
pp. 827-832 ◽  
Author(s):  
Koji Niita ◽  
Y. Iwamoto ◽  
T. Sato ◽  
N. Matsuda ◽  
Y. Sakamoto ◽  
...  

2005 ◽  
Vol 35 (2) ◽  
pp. 208-213 ◽  
Author(s):  
T. Sato ◽  
L. Sihver ◽  
H. Iwase ◽  
H. Nakashima ◽  
K. Niita

2011 ◽  
Vol 2011 ◽  
pp. 1-12 ◽  
Author(s):  
S. R. Hashemi-Nezhad ◽  
M. Zamani-Valasiadou ◽  
M. I. Krivopustov ◽  
R. Brandt ◽  
W. Ensinger ◽  
...  

The neutron production in thick targets irradiated with 1 GeV protons was studied experimentally, and results are well understood with model calculations, including MCNPX 2.7a. However, one observes very large neutron production rates in the interaction of 44 GeV 12C onto thick Cu-, Pb-, and U-targets beyond calculated rates. The experimental spallation product yield curve in a 20 cm thick Cu target irradiated with 72 GeV 40Ar also cannot be reproduced by several model codes, including MCNPX 2.7a. This may be due to secondary fragments produced in high energy ( GeV) heavy-ion interactions which destroy target nuclei more effectively than primary ions. These observed experimental facts constitute “unresolved problems” from a fundamental point of view. It may have an impact on radiation protection issues for future heavy-ion accelerators.


2020 ◽  
Vol 65 (6) ◽  
pp. 065004
Author(s):  
Thunyarat Chusin ◽  
Kosuke Matsubara ◽  
Akihiro Takemura ◽  
Rena Okubo ◽  
Yoshinori Ogawa

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