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Distribution of r_(12) ? p_(12) in quantum systems

机译:r_(12)的分布?量子系统中的p_(12)

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摘要

We introduce the two-particle probability density X(x) of x = r_(12) ? p_(12) = (r_1 ? r_2) ? (p_1? p_2). The fundamental equations involved in the derivation of this new intracule X(x), which we call the Posmom intracule, are derived and we show how to derive X(x) from the many-particle wave-function. We contrast it with the Dot intracule [Y.A. Bernard, D.L. Crittenden, and P.M.W. Gill, Phys. Chem. Chem. Phys. 10, 3447 (2008)] which can be derived from the Wigner distribution and show the relationships between the Posmom intracule and the one-particle Posmom density [Y.A. Bernard, D.L. Crittenden, and P.M.W. Gill, J. Phys. Chem. A 114, 11984 (2010)]. To illustrate the information provided by the Posmom intracule, we apply this new formalism to various two-electron systems: the three-dimensional parabolic quantum dot, the helium-like ions and the ground and excited states of the helium atom.
机译:我们引入x = r_(12)?的两粒子概率密度X(x)? p_(12)=(r_1?r_2)? (p_1?p_2)。推导了涉及此新粒子X(x)推导的基本方程式,我们称其为Posmom粒子,并展示了如何从多粒子波函数推导X(x)。我们将其与点状分子[Y.A.伯纳德·D·L Crittenden和P.M.W.吉尔,物理学。化学化学物理10,3447(2008)]可从Wigner分布中得出,并显示了Posmom内在分子与单颗粒Posmom密度之间的关系[Y.A.伯纳德·D·L Crittenden和P.M.W. Gill,J.Phys。化学A 114,11984(2010)。为了说明Posmom微粒提供的信息,我们将此新形式主义应用于各种两电子系统:三维抛物线量子点,类氦离子以及氦原子的基态和激发态。

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