{"title":"铯中电偶极子极化率和核自旋相关奇偶性不守恒的福克空间扰动相对论耦合簇计算","authors":"Suraj Pandey, Ravi Kumar, D. Angom, B. K. Mani","doi":"arxiv-2408.04356","DOIUrl":null,"url":null,"abstract":"We implement the Fock-space perturbed relativistic coupled-cluster theory to\ncompute the electric dipole polarizability of ground and low lying excited\nstates, and nuclear spin-dependent parity violating transition amplitudes in\nCs. Moreover, to check the accuracy of the wavefunctions used in the\ncalculations, we compute the excitation energies, E1 transition amplitudes and\nmagnetic dipole hyperfine constants for ground and low lying excited states. To\nimprove the accuracy of the computed properties, we have incorporated the\ncorrections from the relativistic and QED effects in our calculations. The\ncontributions from triple excitations are accounted perturbatively. Our results\non excitation energies, E1 transition amplitudes and hyperfine constants are in\ngood agreement with the experimental results. Our polarizability results using\nFS-PRCC theory are in good agreement with the experimental data. Our values of\nparity-violating transition amplitudes are, in general, on the lower side of\nthe previous values. From the analysis of the electron correlations, we find\nthat the corrections from the Breit interaction and QED effects are important\nto get accurate results of nuclear spin-dependent parity-violating transition\namplitudes in Cs. The largest cumulative contribution from Breit and QED\ncorrections is found to be $\\approx$ 3.2\\% of the total value. The upper bound\non the theoretical uncertainty in our calculated parity violating transition\namplitudes is estimated to be about 1\\%.","PeriodicalId":501039,"journal":{"name":"arXiv - PHYS - Atomic Physics","volume":"22 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Fock-space perturbed relativistic coupled-cluster calculations of electric dipole polarizability and nuclear spin-dependent parity non-conservation in Cs\",\"authors\":\"Suraj Pandey, Ravi Kumar, D. Angom, B. K. Mani\",\"doi\":\"arxiv-2408.04356\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We implement the Fock-space perturbed relativistic coupled-cluster theory to\\ncompute the electric dipole polarizability of ground and low lying excited\\nstates, and nuclear spin-dependent parity violating transition amplitudes in\\nCs. Moreover, to check the accuracy of the wavefunctions used in the\\ncalculations, we compute the excitation energies, E1 transition amplitudes and\\nmagnetic dipole hyperfine constants for ground and low lying excited states. To\\nimprove the accuracy of the computed properties, we have incorporated the\\ncorrections from the relativistic and QED effects in our calculations. The\\ncontributions from triple excitations are accounted perturbatively. Our results\\non excitation energies, E1 transition amplitudes and hyperfine constants are in\\ngood agreement with the experimental results. Our polarizability results using\\nFS-PRCC theory are in good agreement with the experimental data. Our values of\\nparity-violating transition amplitudes are, in general, on the lower side of\\nthe previous values. From the analysis of the electron correlations, we find\\nthat the corrections from the Breit interaction and QED effects are important\\nto get accurate results of nuclear spin-dependent parity-violating transition\\namplitudes in Cs. The largest cumulative contribution from Breit and QED\\ncorrections is found to be $\\\\approx$ 3.2\\\\% of the total value. The upper bound\\non the theoretical uncertainty in our calculated parity violating transition\\namplitudes is estimated to be about 1\\\\%.\",\"PeriodicalId\":501039,\"journal\":{\"name\":\"arXiv - PHYS - Atomic Physics\",\"volume\":\"22 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-08-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Atomic Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2408.04356\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Atomic Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.04356","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
我们利用福克空间扰动相对论耦合簇理论来计算铯的基态和低层激发态的电偶极子极化率,以及核自旋相关的违反奇偶性的转变幅度。此外,为了检验计算中使用的波函数的准确性,我们还计算了基态和低层激发态的激发能、E1 过渡振幅和磁偶极子超细常数。为了提高计算结果的准确性,我们在计算中加入了相对论效应和 QED效应的校正。对三重激发的贡献进行了微扰计算。我们对激发能量、E1 转变振幅和超细常数的计算结果与实验结果非常吻合。我们利用 FS-PRCC 理论得出的极化率结果与实验数据十分吻合。我们得出的违反偏振的转变振幅值总体上偏低。通过对电子相关性的分析,我们发现布赖特相互作用和 QED 效应的修正对于获得 Cs 中核自旋相关的违反奇偶性转变振幅的精确结果非常重要。我们发现布雷特和QED修正的最大累积贡献约为总值的3.2%。我们计算出的违反奇偶性转变幅度的理论不确定性上限估计约为1%。
Fock-space perturbed relativistic coupled-cluster calculations of electric dipole polarizability and nuclear spin-dependent parity non-conservation in Cs
We implement the Fock-space perturbed relativistic coupled-cluster theory to
compute the electric dipole polarizability of ground and low lying excited
states, and nuclear spin-dependent parity violating transition amplitudes in
Cs. Moreover, to check the accuracy of the wavefunctions used in the
calculations, we compute the excitation energies, E1 transition amplitudes and
magnetic dipole hyperfine constants for ground and low lying excited states. To
improve the accuracy of the computed properties, we have incorporated the
corrections from the relativistic and QED effects in our calculations. The
contributions from triple excitations are accounted perturbatively. Our results
on excitation energies, E1 transition amplitudes and hyperfine constants are in
good agreement with the experimental results. Our polarizability results using
FS-PRCC theory are in good agreement with the experimental data. Our values of
parity-violating transition amplitudes are, in general, on the lower side of
the previous values. From the analysis of the electron correlations, we find
that the corrections from the Breit interaction and QED effects are important
to get accurate results of nuclear spin-dependent parity-violating transition
amplitudes in Cs. The largest cumulative contribution from Breit and QED
corrections is found to be $\approx$ 3.2\% of the total value. The upper bound
on the theoretical uncertainty in our calculated parity violating transition
amplitudes is estimated to be about 1\%.