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兆电子伏能区 149Sm(n,α)146Nd 截面。

149Sm(n,α)146Nd cross sections in the MeV region.

机构信息

State Key Laboratory of Nuclear Physics and Technology, Institute of Heavy Ion Physics, Peking University, Beijing 100871, China.

出版信息

Phys Rev Lett. 2011 Dec 16;107(25):252502. doi: 10.1103/PhysRevLett.107.252502. Epub 2011 Dec 14.

Abstract

We have measured the (149)Sm(n,α)(146)Nd cross section at 4.5, 5.0, 5.5, 6.0, and 6.5 MeV. Measurements were performed at the 4.5 MV Van de Graaff accelerator of Peking University with monoenergetic neutrons produced via the (2)H(d,n)(3)He reaction using a deuterium gas target. Alpha particles were detected with a double-section gridded ionization chamber having two back-to-back (149)Sm(2)O(3) samples attached to the common cathode. Absolute neutron flux was measured using a small (238)U fission chamber and monitored by a BF(3) long counter. These are the first reported cross sections for this reaction at these energies, except at 6.0 eV, where our new data are in good agreement with our earlier result. The present results help to much better constrain the (149)Sm(n,α)(146)Nd cross section in a region where its energy dependence is changing fairly rapidly and there are large differences between evaluated nuclear data libraries.

摘要

我们已经测量了 (149)Sm(n,α)(146)Nd 在 4.5、5.0、5.5、6.0 和 6.5 MeV 的截面。这些测量是在北京大学生命科学学院的 4.5 MV 范德格拉夫加速器上进行的,使用氘气体靶通过 (2)H(d,n)(3)He 反应产生单能中子。α粒子是用一个带有两个背对背 (149)Sm(2)O(3)样品的双节网格电离室检测的,这些样品连接到共同的阴极。绝对中子通量是使用一个小的 (238)U 裂变室测量的,并由 BF(3)长计数器进行监测。除了在 6.0 eV 处,这些是这些能量下该反应的首次报道截面,我们的新数据与我们早期的结果非常吻合。目前的结果有助于更好地约束 (149)Sm(n,α)(146)Nd 在其能量依赖性变化相当快且评估核数据库之间存在较大差异的区域的截面。

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