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A general formula for Rayleigh-Schrödinger perturbation energy utilizing a power series expansion of the quantum mechanical Hamiltonian

J. M. Herbert
Technical Memorandum No. 222, Mathematics and Computer Science Division, Argonne National Laboratory (1997)

Abstract

Perturbation theory has long been utilized by quantum chemists as a method for approximating solutions to the Schrödinger equation. Perturbation treatments represent a system's energy as a power series in which each additional term further corrects the total energy; it is therefore convenient to have an explicit formula for the nth-order energy correction term. If all perturbations are collected into a single Hamiltonian operator, such a closed-form expression for the nth-order energy correction is well known; however, use of a single perturbed Hamiltonian often leads to divergent energy series, while superior convergence behavior is obtained by expanding the perturbed Hamiltonian in a power series. This report presents a closed-form expression for the nth-order energy correction obtained using Rayleigh-Schrödinger perturbation theory and a power series expansion of the Hamiltonian.

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