Isotope production in proton-, deuteron-, and carbon-induced reactions on Nb93 at 113 MeV/nucleon
Isotope production in proton-, deuteron-, and carbon-induced reactions on Nb93 at 113 MeV/nucleon
复制标题
Nb93 上 113 MeV/核子的质子、氘核和碳诱导反应中的同位素产生
DOI:
10.1103/physrevc.100.044605
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发表时间:
2019
影响因子:
3.1
通讯作者:
Kondo Yosuke et al.
中科院分区:
文献类型:
--
作者:
Nakano Keita;Watanabe Yukinobu;Kawase Shoichiro;Kondo Yosuke et al.
Isotope-production cross sections for-,-, and C-induced spallation reactions onat 113 MeV/nucleon were measured using the inverse-kinematics method employing secondary targets of,, and C. The measured cross sections for,,produced by-induced reactions were found to be consistent with those measured by the conventional activation method. We performed benchmark tests of the reaction models INCL-4.6, JQMD, and JQMD-2.0 implemented in the Particle and Heavy Ion Transport code System (PHITS) and of the nuclear data libraries JENDL-4.0/HE, TENDL-2017, and ENDF/B-VIII.0. The model calculations also showed generally good agreement with the measured isotope-production cross sections for-,-, and C-induced reactions. It also turns out that, among the three nuclear data libraries, JENDL-4.0/HE provides the best agreement with the measured data for the-induced reactions. We compared the presentdata with thedata, that were measured previously by the same inverse kinematics method (Kawaseet al., Prog. Theor. Exp. Phys. 2017, 093D03 (2017)2050-391110.1093/ptep/ptx110), with particular attention to the effect of neutron-shell closure on isotope production in- and-induced spallation reactions. The isotopic distributions of the measured production cross sections in thedata showed noticeable jumps at neutron numberin the isotopic chains ofand, whereas no such jump appeared in isotopic chain ofin thedata. From INCL-4.6GEM calculations, we found that the jump formed in the evaporation process is smeared out by the intranuclear cascade component inproduced by theandreactions on. Moreover, for, the distribution of the element-production cross sections as a function of the change in proton numberis shifted to smallerthan for, because the excited Nb prefragments generated by the cascade process are more likely to emit protons than the excited Zr prefragments, due to the smaller proton-separation energies of the Nb isotopes.