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1991
DOI: 10.1088/0031-8949/43/1/003
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1/Nenergy-formulae for relativistic two-body Coulomb and Yukawa systems with arbitrary masses

Abstract: Energy formulae for two-particle Klein-Gordon systems subjected to Coulomb and Yukawa potentials are derived to first l/N-order. The energies obtained in this manner incorporate the influence of the mass-asymmetry via the parameter 6 = (M:mi)*. Certain Coulomb-inspired extrapolations to Dirac-particle systems, having the meaning of dominant contributions, are taken into account. Numerical results are presented.

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Cited by 6 publications
(1 citation statement)
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“…Yukawa potential [7][8][9][10][11][12][13][14][15] has also received a great deal of attention in view of the methods by which the potential has been studied. Some of them used to solving the wave equations are the 1/N -expansion [16] and shifted 1/N -expansion methods [17], studying the potential by using the Raygleih-Schrödinger perturbation expansion [18], a group-theoretical approach by using the Fock transformation [3], the variational self-consistent field molecular-orbital method [18], the J-matrix method [19], a new approximation scheme proposed to study the bound states of potential [20], studying in terms of the hypervirial theorems [21] and a numerical solution of the Schrödinger equation for the present potential [22].…”
Section: Introductionmentioning
confidence: 99%
“…Yukawa potential [7][8][9][10][11][12][13][14][15] has also received a great deal of attention in view of the methods by which the potential has been studied. Some of them used to solving the wave equations are the 1/N -expansion [16] and shifted 1/N -expansion methods [17], studying the potential by using the Raygleih-Schrödinger perturbation expansion [18], a group-theoretical approach by using the Fock transformation [3], the variational self-consistent field molecular-orbital method [18], the J-matrix method [19], a new approximation scheme proposed to study the bound states of potential [20], studying in terms of the hypervirial theorems [21] and a numerical solution of the Schrödinger equation for the present potential [22].…”
Section: Introductionmentioning
confidence: 99%