A simple variational approach to perturbation theory is presented which contains as special cases the Goldhammer-Feenberg refinement of the Brillouin-Wigner series, the corresponding refinement of the Rayleigh-Schr\"odinger series, as well as the continued-fraction expansion of the resolvent matrix element. The approach is very effective and works for arbitrary coupling strengths. The method is applied to one-electron atoms, taking the whole Coulomb attraction -Z/r as a perturbation. Already with the first-order wave function, one obtains 99.3% of the exact ground-state energy for all Z. With the second-order wave function one obtains 99.96% of the exact ground-state energy and 99.6% of the exact energy of the first excited state, again for all Z. In the present example the numerical effort is comparable to the one needed to perform the Rayleigh-Schr\"odinger expansion to the corresponding order of the wave function.
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Cederbaum et al. (1975) studied this question.
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