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Relativistic corrections to the partial wave expansion of two-electron atoms

机译:对两个电子原子的部分波扩展的相对论校正

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摘要

The asymptotic behavior of the partial wave expansion (or the Cl expansion in terms of AOs with angular quantum number 1) of the leading relativistic correction for two-electron atomic ions in a S-1 state is studied analytically In agreement with earlier numerical findings, the partial wave increments of the leading relativistic correction go as (l + 1/2)(-2), whereas the nonrelativistic increments go as (l + 1/2)(-4). The coefficient of the leading term is 2 alpha(2)pi(2) integral(infinity)(0)vertical bar psi(r,r,0)vertical bar(2)r(2)dr for the Dirac Coulomb operator, and surprisingly also the full Dirac-Breit operator, while the Gaunt term gives a contribution of -4 alpha(2)pi(2) integral(infinity)(0) vertical bar psi(r,r,0)vertical bar(2)r(3)dr. The results obtained here rely entirely on the nonrelativistic correlation cusp, and do not require assumptions on a no-pair projection or a short-range regularization of the electron interaction. They do not give any information on what happens beyond the leading order of relativistic corrections. (c) 2008 Wiley Periodicals, Inc.
机译:分析了研究处于S-1状态的双电子原子离子的相对论性校正的部分波扩展(或用角量子数为1的AO表示的Cl扩展)的渐近行为。前相对论校正的部分波增量为(l + 1/2)(-2),而非相对论校正的部分波增量为(l + 1/2)(-4)。对于Dirac库仑算子,前导项的系数为2 alpha(2)pi(2)积分(无穷大)(0)竖线psi(r,r,0)竖线(2)r(2)dr令人惊讶的是,整个Dirac-Breit算子也是如此,而Gaunt项给出了-4 alpha(2)pi(2)积分(无穷大)(0)垂直栏psi(r,r,0)垂直栏(2)r (3)博士此处获得的结果完全取决于非相对论相关的尖峰,并且不需要对电子相互作用的无对投影或短距离正则化进行假设。他们没有提供有关相对论校正的领先顺序之外的任何信息。 (c)2008 Wiley期刊公司

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