Abstract
The static dipole polarizability α d, i for an arbitrary bound state i of the non-relativistic hydrogen-like atom has been known for a long time from, e.g; the second-order perturbation theory treatment of the Stark effect. A reliable result for the ground state requires both summation over the discrete spectrum and inclusion of the continuum contribution. This continuum contribution is known to decrease for excited states, but a systematic study of this decrease has not been available so far. We present here representative results from a systematic study of α d, i , which was performed as a first test of a new algorithm for the radial integrals involved. Partial sum approximations of the discrete contribution yield the total α d, i with a relative error of less than 1% for all states i with principal quantum number n≥5. Corresponding results for the relativistic case, for which the radial integral algorithm was developed, will be presented elsewhere.
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Dedicated to Professor Hermann Stoll on the occasion of his 60th birthday
An erratum to this article is available at http://dx.doi.org/10.1007/s00214-005-0068-y.
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Koch, V., Andrae, D. Discrete contributions to static dipole polarizabilities of excited bound states of non-relativistic hydrogen-like atoms. Theor Chem Acc 114, 380–386 (2005). https://doi.org/10.1007/s00214-005-0691-7
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DOI: https://doi.org/10.1007/s00214-005-0691-7