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Charge densities for singlet and triplet electron pairs

机译:单线态和三线态电子对的电荷密度

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Analytic properties of charge densities associated with singlet and triplet electron pairs, pg(r) and pl(r), are presented. In an N-electron system with total spin S, distributions rho(0)(r) and rho(1)(r) are independent of the spin projection quantum number M (spin rotation invariance), as opposed to the usual spin-up and spin-down electron densities, rho(0)(r) and rho(1)(r). We derive equations showing that in the case of a wave function which is a spin-eigenfunction, rho(alpha)(r) and rho(beta)(r) are linear combinations of the total charge density rho(r) and the uncompensated spin density rho(s)(r) = [rho(alpha)(r) - rho(beta)(r)]/2M. For a wave function which is not an eigenfunction of S-2, no such relationship exists. In a related discussion, a definition of the high-spin solution corresponding to a given spin-unrestricted Hartree-Fock wave function is proposed, and a notion of effectively unpaired electrons is introduced. The distributions rho(0)(r) and rho(1)(r) are shown not to be invariant under spin coupling between isolated systems. (C) 2000 John Wiley & Sons, Inc. [References: 17]
机译:提出了与单线态和三线态电子对pg(r)和pl(r)相关的电荷密度的分析性质。在具有总自旋S的N电子系统中,与通常的自旋上升相反,分布rho(0)(r)和rho(1)(r)与自旋投影量子数M(自旋旋转不变性)无关自旋电子密度rho(0)(r)和rho(1)(r)。我们得出方程,表明在波动函数为自旋本征函数的情况下,rhoα(r)和rhoβ(r)是总电荷密度rho(r)和未补偿自旋的线性组合密度rho(s)(r)= [rhoα(r)-rhoβ(r)] / 2M。对于不是S-2本征函数的波动函数,不存在这样的关系。在相关讨论中,提出了与给定的自旋无限制Hartree-Fock波函数相对应的高自旋解的定义,并引入了有效不成对电子的概念。 rho(0)(r)和rho(1)(r)的分布在孤立系统之间的自旋耦合下显示为不变。 (C)2000 John Wiley&Sons,Inc. [参考:17]

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