重介子原子超精细结构中核极化效应的微小性对下一代实验的启示

J. Vandeleur, G. Sanamyan, O. R. Smits, I. A. Valuev, N. S. Oreshkina, J. S. M. Ginges
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引用次数: 0

摘要

对μ介子原子的研究重新引起了人们的兴趣,因为它可以提供有关核结构的详细信息。解释测量结果的一个主要限制因素是核极化贡献。我们提出了一种方法,从理论和实验相结合的角度来确定μ介子原子超精细结构的核极化贡献。我们将该方法应用于^{203,205}元钛和^{209}元铋,发现这些系统的核极化贡献很小,而且其大小限制在总超细分裂的10%元以下。我们还使用半分析模型对核极化贡献进行了直接计算,结果表明核极化贡献可能小两个数量级之多。因此,我们得出结论:对μ介子原子超正弦结构的核极化修正并不代表下一代实验的限制因素。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Smallness of the nuclear polarization effect in the hyperfine structure of heavy muonic atoms as a stimulus for next-generation experiments
There is renewed interest in studies of muonic atoms, which may provide detailed information on nuclear structure. A major limiting factor in the interpretation of measurements is the nuclear polarization contribution. We propose a method to determine this contribution to the hyperfine structure in muonic atoms from a combination of theory and experiment for hydrogenlike ions and muonic atoms. Applying the method to $^{203,205}$Tl and $^{209}$Bi, for which there are H-like ion and muonic atom hyperfine experimental data, we find that the nuclear polarization contribution for these systems is small, and place a limit on its size of less than $10\%$ the total hyperfine splitting. We have also performed direct calculations of the nuclear polarization contribution using a semi-analytical model, which indicate that it may be as much as two orders of magnitude smaller. Therefore, we conclude that the nuclear polarization correction to the hyperfine structure of muonic atoms does not represent a limiting factor for next-generation experiments.
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