Abstract
We present summary results of a bound-state perturbation theory for a relativistic spinless (Klein-Gordon) and a relativistic spin-half (Dirac) particle in central fields due to scalar or fourth-component vector-type interactions for an arbitrary bound state. The reduction of the wave equations to Ricatti form enables a decoupling between the pair of coupled first order differential equations on the large and small component Dirac wave functions or a decoupling of the second order differential equation in the Klein-Gordon case. All corrections to the energies and wave functions, including corrections to the positions of the nodes in excited states, are expressed in quadratures in a hierarchical scheme, without the use of either the Green function or the sum over intermediate states.
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Au, C.K. et al. (1983). Perturbation Theory of a Relativistic Particle in Central Fields. In: Malli, G.L. (eds) Relativistic Effects in Atoms, Molecules, and Solids. NATO Advanced Science Institutes Series, vol 87. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-3596-2_20
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