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Measurements of activation cross sections of (n, p) and (n, α) reactions with d-D neutrons in the energy range of 2.1-3.1 MeV

机译:在2.1-3.1 MeV能量范围内用d-D中子对(n,p)和(n,α)反应的活化截面进行测量

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Activation cross sections for (n, p) and (n, α) reactions were measured by the activation method in the energy range of 2.1-3.1 MeV. The irradiated target isotopes were ~(27)Al, ~(41)K, ~(47)Ti, ~(51)V, ~(54)Fe, ~(59)Co, ~(58,61)Ni, ~(65)Cu, ~(67)Zn, ~(69)Ga, ~(79)Br, ~(92)Mo, ~(93)Nb, and ~(96)Ru. The cross sections for ~(41)K (n, p) ~(41)Ar, ~(61)Ni (n, p) ~(61)Co, ~(65)Cu (n, p) ~(65)Ni, ~(67)Zn (n, p) ~(67)Cu, ~(79)Br (n, p) ~(79m)Se, ~(96)Ru (n, p) ~(96m+g)Tc, and ~(69)Ga (n, α) ~(66)Cu reactions were obtained for the first time. Irradiation was from the d-D neutron source of the Fusion Neutronics Source at the Japan Atomic Energy Research Institute. All cross section values were determined relative to those of the ~(115)In (n, n′) ~(115m)In reaction. To obtain reliable activation cross sections, careful attention was paid to correct neutron irradiation and to correct the measurement of induced activity as well as to determine the mean neutron energy at the irradiation positions. To measure weak activity levels, a highly efficient measuring technique with a well-type High Purity Germanium detector was applied to the activities. The present results were compared against the comprehensive evaluated data in JENDL-3.3,-3.2, and-Activation File 96 as well as in ENDF/B-Ⅵ, and FENDL/A-2.0. We concluded that the evaluated data for ~(41)K (n, p) ~(41)Ar, ~(51)V (n, p) ~(51)Ti, ~(61)Ni (n, p) ~(61)Co, ~(79)Br (n, p) ~(79m)Se, ~(96)Ru (n, p) ~(96m+g)Tc, ~(69)Ga (n, α) ~(66)Cu, and ~(93)Nb (n, α) ~(90m)Y reactions were overestimated or underestimated by more than 30%.
机译:(n,p)和(n,α)反应的活化截面通过活化方法在2.1-3.1MeV的能量范围内测量。辐照的目标同位素为〜(27)Al,〜(41)K,〜(47)Ti,〜(51)V,〜(54)Fe,〜(59)Co,〜(58,61)Ni,〜 (65)Cu,〜(67)Zn,〜(69)Ga,〜(79)Br,〜(92)Mo,〜(93)Nb和〜(96)Ru。 〜(41)K(n,p)〜(41)Ar,〜(61)Ni(n,p)〜(61)Co,〜(65)Cu(n,p)〜(65)的横截面Ni,〜(67)Zn(n,p)〜(67)Cu,〜(79)Br(n,p)〜(79m)Se,〜(96)Ru(n,p)〜(96m + g)首次获得Tc和〜(69)Ga(n,α)〜(66)Cu反应。辐射来自日本原子能研究所的聚变中子学源的d-D中子源。相对于〜(115)In(n,n')〜(115m)In反应的横截面值确定所有横截面值。为了获得可靠的活化截面,要特别注意纠正中子辐照和校正诱导活性的测量以及确定辐照位置的平均中子能量。为了测量较弱的活动水平,将具有良好类型的高纯度锗检测器的高效测量技术应用于活动。将当前结果与JENDL-3.3,-3.2和激活文件96以及ENDF /B-Ⅵ和FENDL / A-2.0中的综合评估数据进行比较。我们得出的结论是〜(41)K(n,p)〜(41)Ar,〜(51)V(n,p)〜(51)Ti,〜(61)Ni(n,p)〜的评估数据(61)Co,〜(79)Br(n,p)〜(79m)Se,〜(96)Ru(n,p)〜(96m + g)Tc,〜(69)Ga(n,α)〜 (66)Cu和〜(93)Nb(n,α)〜(90m)Y反应被高估或低估了30%以上。

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