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Analytic solution of the wave equation for an electron in the field of a molecule with an electric dipole moment

机译:具有电偶极矩的分子场中电子的波动方程的解析解

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We relax the usual diagonal constraint on the matrix representation of the eigenvalue wave equation by allowing it to be tridiagonal. This results in a larger representation space that incorporates an analytic solution for the non-central electric dipole potential cos theta/r(2), which was believed not to belong to the class of exactly solvable potentials. Therefore, we were able to obtain a closed form solution of the three-dimensional time-independent Schrodinger equation for a charged particle in the field of a point electric dipole that could carry a nonzero net charge. This problem models the interaction of an electron with a molecule (neutral or ionized) that has a permanent electric dipole moment. The solution is written as a series in a basis composed of special functions that support a tricliagonal matrix representation for the angular and radial components of the wave operator. Moreover, this solution is for all energies, the discrete (for bound states) as well as the continuous (for scattering states). The expansion coefficients of the radial and angular components of the wave-function are written in terms of orthogonal polynomials satisfying three-term recursion relations. For the Coulomb-free case, where the molecule is neutral, we calculate critical values for its dipole moment below which no electron capture is allowed. These critical values are obtained not only for the ground state, where it agrees with already known results, but also for excited states as well. (C) 2007 Elsevier Inc. All rights reserved.
机译:通过让它成为三对角线,我们放宽了特征值波动方程的矩阵表示上通常的对角约束。这导致更大的表示空间,其中包含非中心偶极电势cos theta / r(2)的解析解,据认为这不属于可精确解决的电势类别。因此,我们能够在点电偶极子场中带电粒子的三维时间独立的薛定inger方程的闭合形式解中,该点可以携带非零净电荷。这个问题模拟了电子与具有永久电偶极矩的分子(中性或离子化)的相互作用。该解决方案在一系列特殊功能的基础上写成系列,这些特殊功能支持波算子的角和径向分量的三斜矩阵表示。此外,该解决方案适用于所有能量,包括离散能量(对于束缚态)和连续能量(对于散射态)。波函数的径向和角分量的膨胀系数用满足三项递归关系的正交多项式表示。对于分子为中性的无库仑情况,我们计算了其偶极矩的临界值,在该临界值以下,不允许电子捕获。这些临界值不仅针对与已知结果一致的基态获得,而且还针对激发态获得。 (C)2007 Elsevier Inc.保留所有权利。

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