首页> 外文OA文献 >Calculations of long-range three-body interactions for He($n_0\,^{\lambda}S$)-He($n_0\,^{\lambda}S$)-He($n_0^{\prime}\,^{\lambda}L$)
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Calculations of long-range three-body interactions for He($n_0\,^{\lambda}S$)-He($n_0\,^{\lambda}S$)-He($n_0^{\prime}\,^{\lambda}L$)

机译:计算远程三体相互作用   他($ N_0 \ ^ {\拉姆达} s $) - 他($ N_0 \ ^ {\拉姆达} s $) - 他($ N_0 ^ {\黄金} \ ^ {\拉姆达} L $)

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摘要

We theoretically investigate long-range interactions between an excited $L$state He atom and two identical $S$ state He atoms, for the cases of the threeatoms all in spin singlet states or all in spin triplet states, denoted byHe($n_0\,^{\lambda}S$)-He($n_0\,^{\lambda}S$)-He($n_0^{\prime}\,^{\lambda}L$),with $n_0$ and $n_0'$ principal quantum numbers, $\lambda=1$ or 3 the spinmultiplicity, and $L$ the orbital angular momentum of a He atom. Usingdegenerate perturbation theory for the energies up to second-order, we evaluatethe coefficients $C_3$ of the first order dipolar interactions and thecoefficients $C_6$ and $C_8$ of the second order additive and nonadditiveinteractions. Both the dipolar and dispersion interaction coefficients, forthese three-body degenerate systems, show dependences on the geometricalconfigurations of the three atoms. The nonadditive interactions start to appearin second-order. To demonstrate the results and for applications, the obtainedcoefficients $C_n$ are evaluated with highly accurate variationally-generatednonrelativistic wave functions in Hylleraas coordinates forHe($1\,^{1}S$)-He($1\,^{1}S$)-He($2\,^{1}S$),He${(1\,^{1}S)}$-He${(1\,^{1}S)}$-He${(2\,^{1}P)}$,He${(2\,^{1}S)}$-He${(2\,^{1}S)}$-He${(2\,^{1}P)}$, andHe${(2\,^{3}S)}$-He${(2\,^{3}S)}$-He${(2\,^{3}P)}$. The calculations are givenfor three like-nuclei for the cases of hypothetical infinite mass He nuclei,and of real finite mass $^4{}$He or $^3{}$He nuclei. The special cases of thethree atoms in equilateral triangle configurations are explored in detail, andfor the cases where one of the atoms is in a $P$ state, we also present resultsfor the atoms in an isosceles right triangle configuration or in an equallyspaced co-linear configuration. The results can be applied to constructpotential energy surfaces for three helium atom systems.
机译:我们从理论上研究了激发的$ L $状态He原子和两个相同的$ S $状态He原子之间的远程相互作用,对于三原子都处于自旋单重态或都处于自旋三重态的情况,用He($ n_0 \ ,^ {\ lambda} S $)-He($ n_0 \,^ {\ lambda} S $)-He($ n_0 ^ {\ prime} \,^ {\ lambda} L $),其中$ n_0 $和$ n_0'$个主量子数,$ \ lambda = 1 $或3个自旋多重性,$ L $个He原子的轨道角动量。使用简并摄动理论求解直至二阶的能量,我们评估了一阶偶极相互作用的系数$ C_3 $以及二阶加性和非加性相互作用的系数$ C_6 $和$ C_8 $。所谓的三体简并系统,偶极和色散相互作用系数都显示出对这三个原子的几何构型的依赖性。非加性相互作用开始以二阶形式出现。为了说明结果并进行应用,使用在Hylleraas坐标中针对He($ 1 \,^ {1} S $)-He($ 1 \,^ {1} S $的Hylleraas坐标的高精度变化生成的非相对论波动函数来评估获得的系数$ C_n $。 )-He($ 2 \,^ {1} S $),He $ {(1 \,^ {1} S)} $-He $ {(1 \,^ {1} S)} $-He $ { (2 \,^ {1} P)} $,He $ {(2 \,^ {1} S)} $-He $ {(2 \,^ {1} S)} $-He $ {(2 \,^ {1} P)} $和He $ {(2 \,^ {3} S)} $-He $ {(2 \,^ {3} S)} $-He $ {(2 \, ^ {3} P)} $。对于假设无限质量He核和实有限质量$ ^ 4 {} $ He或$ ^ 3 {} $ He核的情况,给出了三个类似核的计算。详细探讨了等边三角形构型中三个原子的特殊情况,对于其中一个原子处于$ P $状态的情况,我们还给出了等腰直角三角形构型或等距共线的原子的结果组态。该结果可用于构造三个氦原子系统的势能面。

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