类镍Hf~（44＋）、Ta~（45＋）、W~（46＋）、Re~（47＋）、Pt~

本文用多组态Ｄｉｒａｃ－Ｆｏｃｋ（ＭＣＤＦ）法计算了类镍Ｈｆ４４＋、Ｔａ４５＋、Ｗ４６＋、Ｒｅ４７＋、Ｐｔ５０＋、Ａｕ５１＋能级的精细结构和ｎ＝３—４偶极跃迁辐射的振子强度，得到了和实验符合得相当好的结果（对有实验数据的跃迁波长而言），并对组态的选取、核模型的影响、Ｂｒｅｉｔ修正和ＱＥＤ效应作了讨论指出对于本文研究体系，ＱＥＤ效应对跃迁的贡献可以忽略。     

类镍Hf^44＋,Ta^45＋,W^46＋,Re^47＋,Pt^50＋,Au^51＋能级结构…

本文用多组态Ｄｉｒａｃ－Ｆｏｃｋ（ＭＣＤＦ）法计算了类镍Ｈｆ＾４４＋、Ｔａ＾４５＋、Ｗ＾４６＋、Ｒｅ＾４７＋、Ｐｔ＾５０＋、Ａｕ＾５１＋能级的精细结构和ｎ＝３－４偶极跃迁辐射的振子强度，得到了和实验符合得相当好的结果（对有实验数据的跃迁波长而言），并对组态的选取、核模型和、Ｂｒｅｉｔ修正和ＱＥＤ效应作了讨论，指出对于本文研究体系，ＱＥＤ效应对跃迁的贡献可以忽略。     

锶Sr,钡Ba和镭Ra的单光子电四极矩光谱跃迁的理论研究

用带有Ｂｒｅｉｔ和ＱＥＤ修正的全相对论多组态Ｄｉｒａｃ－Ｆｃｃｋ平均能级（ＭＣＤＦ－ＡＬ）模型,计算了碱土金属Ｓｒ、钡Ｂａ和镭Ｒａ的单光子电四极矩＾１Ｄ－＾１Ｓ跃迁的光谱能量间隔,最大跃迁几率和振子强度。计算中考虑了重要的相对论效应、电子关联效应和核的有限体积效应,所得的结果与国外早期发表的结果进行了比较,此外还首次从理论上预言了镭Ｒａ的单光子电四极矩＾１Ｄ－１Ｓ光谱跃迁。     

电子相关对Xe10+离子4d8—4d75p跃迁系跃迁概率的影响

应用多组态Dirac-Fock(MCDF)方法，对Xe¹⁰⁺离子进行了理论计算，获得了跃迁波长和概率等数据.通过逐步引入4dⁿ—5pⁿ(n=1, 2, 3)电子相关的相互作用组态，重点研究了电子相关效应对4d⁸—4d⁷5p跃迁系跃迁概率的影响.结果显示电子相关效应显著，表明了欲得到精确的4d⁸—4d⁷5p的振子强度(跃迁概率)数据，理论计算中至少要包括到4d²—5p²的电子相关组态的影响.与实验测得的跃迁波长比较发现，理论结果与之有着较好的一致性；同时理论跃迁概率在两种规范下的结果符合得相当精确，显示了计算结果的可靠性. 关键词： 多组态Dirac-Fock(MCDF)方法 电子相关 跃迁概率     

类氦离子Cr^22＋精细结构能级和光谱跃迁的相对论多组态 …

采用相对论多组态自洽场方法,计算了Ｃｒ＾２２＋离子的精细结构能级,能级宽度,激发态寿命和光谱跃迁参数。计算中考虑了核的有限体积效应,Ｂｒｅｉｔ修正,ＱＣＤ修正和轨道极化效应。所得结果与文献的实验值和计算值进行了比较。     

~(190─200)Pt偶质量同位素低能激发态的微观研究

从壳模型组态、价核子间有效相互作用及费米子Ｅ２跃迁算子出发，利用一种以Ｄｙｓｏｎ玻色子展开为基础的微观方案，给出了ｓｄｇＩＢＭ－１哈密顿量及玻色子Ｅ２跃迁算子，计算了１９０─２００Ｐｔ偶质量同位素的低激发态能谱及Ｅ２约化跃迁矩阵元，理论计算结果与实验值或唯象工作做了比较，符合较好。     

MoⅩⅣ—RuⅩⅥ离子的3d104s—3d94s4p跃迁谱线波长和振子强度的计算

在对GeⅣ—RuⅩⅥ离子3d-94s4p组态能级结构的组态相互作用理论分析计算的基础上，进一步分析了关联效应，量子电动力学（QED）效应及其他效应对等电子序列离子能级结构的影响，找出了沿等电子序列离子能级变化的规律性.在前人研究工作的基础上，预测计算了MoⅩⅣ—RuⅩⅥ离子3d-94s4pJ=12,32组态能级，由此计算了MoⅩⅣ—RuⅩⅥ离子3d-104s—3d-94s4pJ=12,32跃迁谱线波长，振子强度和跃迁概率. 关键词： GeⅣ—RuⅩⅥ离子 谱线波长 振子强度 跃迁概率     

CuⅩⅧ离子谱线波长和跃迁概率的理论计算

用多组态HFR方法对CuⅩⅧ离子n=3complex组态能级结构进行了综合的分析与计算.在已 有实验工作的基础上，运用参数拟合方法获得了能级结构参数的最佳计算值，由这些参数值 预测计算了CuⅩⅧ离子n=3complex组态能级以及3s²—3s3p,3s3p—3p ²,3p²—3p3d,3s3d—3p3d,3p3d—3d²组态能级跃迁的谱线波 长，振子强度和跃迁概率. 关键词： CuⅩⅧ离子 原子能级 跃迁谱线波长 振子强度和跃迁概率     

类Ne铜离子双电子复合过程辐射跃迁几率的MCDF计算

在组态相互作用的ｊ－ｊ耦合下，用相对论多组态Ｄｉｒａｃ－Ｆｏｃｋ（ＭＣＤＦ）方法计算类Ｎｅ铜离子（２９Ｃｕ１９＋）双电子复合过程的辐射跃迁几率。在计算中涉及了大量的双激发态的和单激发态的相对论组态函数，得出了所有可能的跃迁几率，精选得出最可能的跃迁结果。文中所使用的相对论ＭＣＤＦ方法克服了其他方法诸如在相对论效应、组态相互作用等方面的缺陷，从而获得了很好的结果。所得的结果可用于进一步计算类Ｎｅ铜离子的双电子复合系数     

类氧离子CoⅩⅩ，NiⅩⅪ，CuⅩⅩⅡ和ZnⅩⅩⅢ精细结构能级和跃迁波长的MCDF计算

本文用相对论多组态Ｄｉｒａｃ－Ｆｏｃｋ广义平均能级（ＭＣＤＦ—ＥＡＬ）模型计算了可能成为激光工作物质的类氧离子ＣｏⅩⅩ，ＮｉⅩⅪ，ＣｕⅩⅩⅡ和ＺｎⅩⅩⅢ的４８个精细结构能级和９３个３ｓ—３ｐ跃迁波长。３ｐ组态能级和３ｓ—３ｐ跃迁波长是本文首次预言的。     

类钾离子4s 2S1/2─3d 2D3/2电四极矩E2光谱跃迁的理论研究

采用全相对论量子力学GRASP²程序，广义平均能级EAL模型，在核的有限体积效应，Breit和QED效应的高阶扰动基础上，考虑到原子实的极化，系统地计算了高剥离类钾离子4s ²S_1/2─3d ²D_3/2电四极矩E2光谱跃迁的能级间隔，跃迁概率和振子强度，结果表明：考虑原子实极化效应后，计算的精细能级结构间隔与实验数据之间的系统误差基本消除，其跃迁概率和振子强度属首次报道. 关键词： 高剥离态 能级间隔 振子强度     

Hyperfine induced {\sf 1 s}{\sf 2 s}\ ^{\sf 1}S_{\sf 0} \rightarrow {\sf 1 s}^{\sf 2}\ ^{\sf 1}S0 M1 transition of He-like ions

Hyperfine induced $1s2s\ ^1$ S $_0 \rightarrow 1s^2\ ^1$ S₀ M1 transition probabilities of He-like ions have been calculated from relativistic configuration interaction wavefunctions including the frequency independent Breit interaction and QED effects. Present results for ¹⁵¹Eu and ¹⁵⁵Gd are in good agreement with previous calculations [L.N. Labzowsky et al., Phys. Rev. A 63, 054105 (2001)]. Electronic data are given in terms of a general scaling law in Z that, given isotopic nuclear spin and magnetic moment, allows hyperfine induced decay rates to be estimated for any isotope. The results should be helpful for future experimental investigations on QED and parity non-conservation effects.     

Multiconfiguration Dirac-Fock calculation of transition energies in highly ionized bismuth, thorium, and uranium

Structure and QED effects for and levels are calculated for lithiumlike U⁸⁹⁺ trough neonlike U⁸²⁺, lithiumlike Th⁸⁷⁺ trough neonlike Th⁸⁰⁺ and lithiumlike Bi⁸⁰⁺ trough neonlike Bi⁷³⁺. The results of the first two sets are compared with recent measurements of the transition energy in 3 to 10-electron ions. Good agreement with experiment is found for most of the observed lines. Forty-one possible transitions are calculated for each ion in the eight ionization states, in the experimental energy range. Twenty-eight of these transitions have not been observed, nor calculated previously. We also calculate transition rates, branching ratios, excitation and ionization cross sections and confirm that the thirteen experimental o bserved transitions correspond to the ones with highest relative intensities. However, we find nineteen more transitions that could be measured in a more sensitive experiment. Received: 5 November 1997 / Accepted: 8 December 1997     

类铍离子磁四极M2 2s2 1S0—2s2p3P2 (Z=10—103)禁戒跃迁

利用全相对论多组态Dirac-Fock方法系统地计算了高离化类铍离子的磁四极M2 2s²¹S₀—2s2p³P₂ (Z=10—103)自旋禁戒跃迁的能级间隔、跃迁概率和振子强度，计算中考虑了重要核的有限体积效应，Breit修正和QED修正，所得结果和最近的实验数据以及理论值进行了比较，结果表明：高原子序数的高电荷离子(Z≥70)磁四极M2自旋禁戒跃迁几乎可以和中性原子的光学允许跃迁相比拟，不仅在天体等离子体中，在ICF和MCF高温激光等离子体中，磁四极自旋禁戒跃迁和其他自旋禁戒跃迁（磁偶极、电四极）一样不容忽视，在双电子复合、不透明度、自由程等理论计算中应该考虑其影响. 关键词： 磁四极M2 能级间隔 跃迁概率 振子强度     

Pionic and radiative decays of vector mesons in the chiral bag model

It is shown that a mechanism, within the framework of the cloudy bag model, analogous to that fore ⁺ e ^?→2ψ in QED accounts qualitatively for the decays ?→2π, ω→πψ and ?→πψ with a bag radii 0.8–1.0 fm, and averaged momenta for decay particles. For the radiative decays, the process identical to that in the vector-dominance model gives about 60% of the total calculated width. It also explains small decay widths previously calculated, using the single quark transition process.     

Theoretical study on the 1s22s-1s2 np transitions for Ni25+ ion

The transition energies, wavelengths and oscillator strengths for the 1s²2s-1s² np (n ? 9) transitions of Ni²⁵⁺ ion are calculated. In calculation of the energies, we not only take account of the firstorder corrections from relativistic and mass-polarization effects, but also estimate the higher-order relativistic contribution and QED correction by introducing the effective nuclear charge. The results agree with experimental data available in literature satisfactorily. Grotrian diagram showing these transitions is given.     

Transition wavelengths and probabilities for spectral lines of Zr III

Wavelengths and oscillator strengths for all 4d4f↦4d² dipole-allowed fine-structure transitions in Zr III have been calculated within the Multi-Configuration Dirac-Fock method with QED corrections. These transitions are included in the spectrum of some chemically peculiar stars, like the B-type star χ Lupi observed by the Hubble space telescope. The results are compared to existing experimental and semi-empirical data.     

高离化类铍离子2s21S0—2s2p3P1(Z=10—103)自旋禁戒光谱跃迁

利用全相对论性多组态Dirac-Fock平均能级(MCDF-AL)方法系统地计算了高离化类铍离子自 旋禁戒2s^{2 1}S₀—2s2p³P₁(Z= 10—103)跃迁的能级间隔和跃迁概率,计算中考虑了重要的核的有限体积效应,Breit修正 和QED修正,所得结果和最近的实验数据及理论计算值进行了比较,结果表明：高原子序数 的高荷电离子的自旋禁戒跃迁的跃迁概率和中性原子的电偶极E1的相当,在ICF和MC 关键词： 高离化态 跃迁概率     

Testing of QED-Theory and Precise Measurements of the Rydberg Series for the He-Like Multicharged Ions

The wavelengths of the 1snp ¹ P ₁−1s ^{2 1} S ₀ transitions in He-like Mg XI, F VIII (n= 4–8) and Al XII (n=6,9) have been calculated in the framework of the 1/Z expansion method including relativistic effects and QED contributions. It is found that QED corrections to the ground-state ionization energy are significant at the present level of experimental accuracy. This revised version was published online in July 2006 with corrections to the Cover Date.     

Estimates of the bound-state QED contributions to the g-factor of valence ns electrons in alkali metal atoms

The bound-state QED corrections to g-factors are partly calculated and partly estimated for the ns valence electrons in the atoms K, Rb, Cs, Ba⁺ and Fr. It is shown that these corrections should be taken into account in the comparison with experimental data.