Dimensional interpolation for two-electron atoms

114Citations
Citations of this article
11Readers
Mendeley users who have this article in their library.
Get full text

Abstract

The ground-state electronic energy of helium-like atoms is calculated by interpolating between exact solutions for the limiting cases of one-dimensional and infinite-dimensional systems. In suitably scaled coordinates, the D=1 limit corresponds to replacing the Coulombic potentials by delta functions. With another choice of scaling, the D=∞ limit reduces to a classical electrostatic problem; the electrons take fixed positions that correspond to replacing wave functions with delta functions. The ground-state energy for arbitrary dimension D and nuclear charge Z can be represented as εD=ε∞ [1+c1/D+c 2/D2+F(D,Z)/D3]. The first three terms are obtained from a perturbation expansion about D=∞; these correspond, respectively, to the limiting rigid electronic structure (envisioned by G. N. Lewis!) and to harmonic and anharmonic vibrations about that structure. The interpolation function F(D,Z) is approximated as a geometric series, determined by fitting the accurately known energies for the D=1 limit and for D=5. This procedure yields an accuracy of 2 parts in 105 or better for D=3 and Z≥2. Study of the Z dependence reveals that at D=1 the perturbation expansion in powers of 1/Z has a self-similar structure. Also, for each D there exists a critical nuclear charge Z*, with magnitude near 12, for which F(D,Z*)=0; the first three terms of the expansion about D=∞ then give the exact energy. © 1986 American Institute of Physics.

Cite

CITATION STYLE

APA

Herschbach, D. R. (1986). Dimensional interpolation for two-electron atoms. The Journal of Chemical Physics, 84(2), 838–851. https://doi.org/10.1063/1.450584

Register to see more suggestions

Mendeley helps you to discover research relevant for your work.

Already have an account?

Save time finding and organizing research with Mendeley

Sign up for free