paper

Static electric multipole susceptibilities of the relativistic hydrogen-like atom in the ground state: Application of the Sturmian expansion of the generalized Dirac-Coulomb Green function

arXiv:1602.00613 · doi:10.1103/PhysRevA.93.062502

Abstract

The ground state of the Dirac one-electron atom, placed in a weak, static electric field of definite -polarity, is studied within the framework of the first-order perturbation theory. The Sturmian expansion of the generalized Dirac-Coulomb Green function [R. Szmytkowski, J. Phys. B 30 (1997) 825, erratum: 30 (1997) 2747] is used to derive closed-form analytical expressions for various far-field and near-nucleus static electric multipole susceptibilities of the atom. The far-field multipole susceptibilities --- the polarizabilities , electric-to-magnetic cross-susceptibilities and electric-to-toroidal-magnetic cross-susceptibilities --- are found to be expressible in terms of one or two non-terminating generalized hypergeometric functions with the unit argument. Counterpart formulas for the near-nucleus multipole susceptibilities --- the electric nuclear shielding constants , near-nucleus electric-to-magnetic cross-susceptibilities and near-nucleus electric-to-toroidal-magnetic cross-susceptibilities --- involve terminating series and for each may be rewritten in terms of elementary functions. Exact numerical values of the far-field dipole, quadrupole, octupole and hexadecapole susceptibilities are provided for selected hydrogenic ions. Analytical quasi-relativistic approximations, valid to the second order in , where is the fine-structure constant and is the nuclear charge number, are derived for all types of the far-field and near-nucleus susceptibilities considered in the paper.

66 pages, 19 tables

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