\(^{129}\) Xe, \(^{199}\) Hg, \(^{223}\) Rn, \(^{225}\) Ra和\(^{171}\) Yb原子中电偶极矩的相对论多体计算

Y. Singh, B. Sahoo
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引用次数: 0

摘要

我们提出并比较了由于核席夫矩(NSM)和原子核与电子之间的张量-伪张量(T-PT)相互作用而导致的各种闭壳原子的永久电偶极矩(EDMs)的结果。为了突出电子相关效应在获得精确电火花加工结果中的作用,我们在不同近似程度上采用了包括耦合簇理论在内的相对论多体方法。结合我们从单激发和双激发水平(CCSD方法)的相对论耦合簇(RCC)得到的结果与可用的EDM测量结果,我们得到了与各自的NSM和T-PT相互作用相关的耦合的精确边界\(S\)和\(C_T\)。结合我们的CC结果,对\(^{199}\) Hg的最精确的电火花加工测量结果分别为\(S<1.45 \times 10^{-12}|e|\) fm \(^3\)和\(C_T < 2.09 \times 10^{-9}\)。进一步将这些边界与最新的核结构和量子色动力学计算相结合,我们推断出强cp违反参数和组合的上、下夸克色edm的极限分别为\(|\bar{\theta}| < 1.1 \times 10^{-9}\)和\(|\widetilde{d}_u - \widetilde{d}_d| < 2.8 \times 10^{-26} |e|\) cm。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Relativistic Many-body Calculations for Electric Dipole Moments in \(^{129}\)Xe, \(^{199}\)Hg, \(^{223}\)Rn, \(^{225}\)Ra and \(^{171}\)Yb Atom
We present and compare the results of permanent electric dipole moments (EDMs) of various closed-shell atoms due to the nuclear Schiff moment (NSM) and the tensor-pseudotensor (T-PT) interactions between the atomic nuclei and electrons. In order to highlight the role of electron-correlation effects in obtaining accurate EDM results, we employ a number of relativistic many-body methods including coupled-cluster theory at different degrees of approximation. On combining our results obtained from the relativistic coupled-cluster (RCC) at the levels of singles and doubles excitations (CCSD method) with the available EDM measurements we obtain accurate bounds on the couplings \(S\) and \(C_T\) associated with the respective NSM and T-PT interactions. The most precise EDM measurement on \(^{199}\)Hg in combination with our CC results yield limits on the above couplings as \(S<1.45 \times 10^{-12}|e|\)fm\(^3\) and \(C_T < 2.09 \times 10^{-9}\) respectively. Further combining these bounds with the latest nuclear structure and quantum chromodynamics calculations we infer limits on the strong CP-violating parameter and for the combined up- and down- quark chromo-EDMs as \(|\bar{\theta}| < 1.1 \times 10^{-9}\) and \(|\widetilde{d}_u - \widetilde{d}_d| < 2.8 \times 10^{-26} |e|\)cm, respectively.
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