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首页> 外文期刊>European Physical Journal Plus >Atomic data of intermediate autoionzing Rydberg series nf[K](J) (n=4, 5), nd[K](J) (n=5, 6), np[K](J) (n=6, 7) and ns[K](J) (n=7, 8) of neutral argon atom in the multiconfiguration Dirac-Hartree-Fock framework
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Atomic data of intermediate autoionzing Rydberg series nf[K](J) (n=4, 5), nd[K](J) (n=5, 6), np[K](J) (n=6, 7) and ns[K](J) (n=7, 8) of neutral argon atom in the multiconfiguration Dirac-Hartree-Fock framework

机译:中间体自动化rydberg系列NF [k](j)(n = 4,5),nd [k](j)(n = 5,6),np [k](n = 6,7)的原子数据 在多组配置Dirac-hartree-Fock框架中,NS [K](J)(n = 7,8)中性氩气原子

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We report the results of an accurate computation of the energy levels, oscillator strengths f(ij), the radiative transition rates A(ij), the Lande g-factor, the magnetic dipole and the electric quadrupole hyperfine constants of the intermediate Rydberg series nf[K](J) (n = 4, 5), nd[K](J) (n = 5, 6), np[K](J) (n = 6, 7) and ns[K](J) (n = 7, 8) relative to the ground state 3p(6) S-1(0) for neutral argon atom spectra based on the multiconfiguration Dirac-Hartree-Fock (MCDHF) approach. In this approach, the quantum electrodynamics (QED) effects with transverse photon Breit interaction and vacuum photon polarization self-energy corrections are included. Moreover, the perturbation due to the core-polarization and electron correlation effects are taken into account. We also reported the oscillator strengths and transition rates in Coulomb and Babushkin gauges for the 3p(5) (P-2)3d-3p(5) (P-2)4f-3p(5) (P-2)3d-3p(5) (P-2)5f-3p(5) (P-2)4d-3p(5) (P-2)4f-3p(5) (P-2)4d-3p(5) (P-2)5f-3p(5) (P-2)5d-3p(5) (P-2)4f-3p(5) (P-2)5d-3p(5) (P-2)5f-3p(5) (P-2)6d-3p(5) (2 P)4f and 3p(5) (P-2)6d-3p(5) (P-2)5f transition arrays as well as the 3p(5) (P-2)5d-3p(5) (P-2)6p, 3p(5) (P-2)7s-3p(5) (P-2)6p, 3p(5) (P-2)7s-3p(5) (P-2)7p and 3p(5) (P-2)8s-3p(5) (P-2)7p transition arrays. Insofar as experimental or theoretical values by other authors exist, comparison is made with those values; it turns out that, for most of the levels, a rather satisfying agreement with these experimental and theoretical results is obtained, thus confirming the reliability of our data.
机译:我们报告了精确计算的能量水平,振荡器强度F(IJ),辐射转变速率A(IJ),Lande G因子,磁性偶极子和中间rydberg系列NF的电偶孔常数[k](j)(n = 4,5),nd [k](j)(n = 5,6),np [k](j)(n = 6,7)和ns [k](j )(n = 7,8)相对于基于多组配置Dirac-Hartree-Fock(MCDHF)方法的中性氩基原子谱相对于地态3P(6)S-1(0)。在这种方法中,包括横向光子空白相互作用和真空光子偏振自能校正的量子电动电动电动(QED)效应。此外,考虑了由于芯极化和电子相关效应引起的扰动。我们还报告了3P(5)(P-2)3D-3P(5)(P-2)4F-3P(5)(P-2)3D-3P中的库仑和Babushkin仪中的振荡器强度和过渡速率(5)(P-2)5F-3P(5)(P-2)4D-3P(5)(P-2)4F-3P(5)(P-2)4D-3P(5)(P- 2)5F-3P(5)(P-2)5D-3P(5)(P-2)4F-3P(5)(P-2)5D-3P(5)(P-2)5F-3P( 5)(p-2)6d-3p(5)(2 p)4f和3p(5)(p-2)6d-3p(5)(p-2)5f过渡阵列以及3p(5) (P-2)5D-3P(5)(P-2)6p,3p(5)(p-2)7s-3p(5)(p-2)6p,3p(5)(p-2)7s -3P(5)(P-2)7P和3P(5)(P-2)8S-3P(5)(P-2)7P过渡阵列。作为其他作者的实验或理论价值存在,与这些值进行比较;事实证明,对于大多数水平,获得了与这些实验和理论结果的相当满意的协议,从而确认了我们的数据的可靠性。

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