Abstract

A computationally facile super convergent perturbation theory for the energies and wavefunctions of the bound states of one-dimensional anharmonic oscillators is suggested. The proposed approach uses a Kolmogorov repartitioning of the Hamiltonian with perturbative order. The unperturbed and perturbed parts of the Hamiltonian are defined in terms of projections in Hilbert space, which allows for zero-order wavefunctions that are linear combinations of basic functions. The method is demonstrated on quartic anharmonic oscillators using a basis of generalized coherent states and, in contrast to usual perturbation theories, converges absolutely. Moreover, the method is shown to converge for excited states, and it is shown that the rate of convergence does not deteriorate appreciably with excitation.

Department(s)

Chemistry

Comments

National Science Foundation, Grant CHE-9975429

Keywords and Phrases

Perturbation theory; Quantum mechanical oscillators; Superconvergence; Time-independent Schrödinger equation

International Standard Serial Number (ISSN)

0259-9791

Document Type

Article - Journal

Document Version

Citation

File Type

text

Language(s)

English

Rights

© 2024 Springer, All rights reserved.

Publication Date

01 Dec 2002

Included in

Chemistry Commons

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