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理论物理通讯:英文版

Hooke's Atom in an Arbitrary External Electric Field: Analytical Solutions of Two-Electron Problem by Path Integral Approach

蔡亮, 张萍, 杨涛, 潘孝胤

Published Jan 1, 2011• 0 citations
OpenAlex

Abstract

由使用路径积分途径,我们在一个任意的时间依赖者电场调查胡克的原子(在一个外部泛音振荡器潜力与库仑潜力交往的二个电子) 的问题。为分离振荡器频率的某个无限的集合,我们获得分析答案。原子的扎根的州的极化当时是计算的。一样的结果也通过线性反应理论被获得。

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由使用路径积分途径,我们在一个任意的时间依赖者电场调查胡克的原子(在一个外部泛音振荡器潜力与库仑潜力交往的二个电子) 的问题。为分离振荡器频率的某个无限的集合,我们获得分析答案。原子的扎根的州的极化当时是计算的。一样的结果也通过线性反应理论被获得。
The system of two interacting electrons in one-dimensional harmonic potential or Hooke’s atom is considered, again. On one hand, it appears as a model for quantum dots in a strong confinement regime, and on the other hand, it provides us with a hard test bench for new methods with the “space splitting” arising from the one-dimensional Coulomb potential. Here, we complete the numerous previous studies of the ground state of Hooke’s atom by including the excited states and dynamics, not considered earlier. With the perturbation theory, we reach essentially exact eigenstate energies and wave functions for the strong confinement regime as novel results. We also consider external perturbation induced quantum dynamics in a simple separable case. Finally, we test our novel numerical approach based on real-time path integrals (RTPIs) in reproducing the above. The RTPI turns out to be a straightforward approach with exact account of electronic correlations for solving the eigenstates and dynamics without the conventional restrictions of electronic structure methods.
Path integral Monte Carlo simulations have been carried out for a system of interacting fermionic particles in one dimension. Due to the fact that the sign problem can be completely eliminated for one-dimensional systems, such simulations allow one to obtain accurate energies and particle densities in arbitrary external potentials. Two cases were considered: electrons in the field of a uniform neutralizing background and in an effective field of atoms on a lattice. In the latter case, a clear asymmetry of the charge density distribution of conducting electrons and holes has been observed.