发现巨大的88Zr中子捕获截面的起源,并量化其对应用的影响

Athanasios Stamatopoulos, Paul Koehler, Andrew Cooper, Aaron Couture, Brad DiGiovine, Artem Matyskin, Veronika Mocko, Jonathan Morrell, Ellen O'Brien, Christiaan Vermeulen
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引用次数: 0

摘要

放射性88 Zr核(83.4天半衰期)在共振能量上吸收中子的概率-它的中子俘获共振积分-是迄今为止报道的最大的,这意味着在与核试验诊断和核合成应用相关的能量上,中子俘获截面比以前认为的要大几个数量级。然而,这些应用需要横截面在能量范围内的形状,而不仅仅是这个积分量。我们在0.0253 ~ 500 eV范围内测量了88zr中子的总截面。因为负责中子俘获截面的相同共振或其他核结构反映在总截面中,我们使用这些数据从后者中提取出前者作为能量的函数。我们的数据显示了在0.171 eV下的共振,并产生了771,000±31,000 barns的热中子捕获截面,与最近公布的值吻合得很好。相比之下,从我们的数据中提取的中子捕获共振积分为15,210±670谷仓,比最近报道的值小200倍。我们将讨论这种差异对应用程序的影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Discovery of the origin of the enormous 88Zr neutron-capture cross section and quantifying its impact on applications
Abstract The probability for a radioactive 88 Zr nucleus (83.4 day half life) to absorb neutrons across resonance energies — its neutron-capture resonance integral — is the largest ever reported and implies that the neutron-capture cross section is orders of magnitude larger than previously thought at energies relevant to nuclear test diagnostics and nucleosynthesis applications. However, these applications require the shape of this cross section across a range of energies, not just this integral quantity. We measured the 88 Zr neutron total cross section from 0.0253 to 500 eV. Because the same resonances or other nuclear structure responsible for the neutron capture-cross section are reflected in the total cross section, we used these data to extract the former from the latter as a function of energy. Our data reveal a resonance at 0.171 eV and result in a thermal neutron-capture cross section of 771,000±31,000 barns, in good agreement with the recently published value. In contrast, the neutron-capture resonance integral extracted from our data, 15,210±670 barns, is a factor of 200 smaller than the recently reported value. We discuss the impact of this difference on applications.
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