Abstract

For further insight into the perturbation technique within the framework of the asymptotic iteration method (PAIM), we suggest this method to be used as an alternative method to the traditional well-known perturbation techniques. We show by means of very simple algebraic manipulations that PAIM can be directly applied to obtain the symbolic expectation value of any perturbed potential piece without using the eigenfunction of the unperturbed problem. One of the fundamental advantages of PAIM is its ability to extract a reference unperturbed potential piece or pieces from the total Hamiltonian which can be solved exactly within AIM. After all, one can easily compute the symbolic expectation values of the remaining potential pieces. As an example, the present scheme is applied to the semi-relativistic wave equation with the harmonic-oscillator potential implemented with the Fermi–Breit potential terms. In particular, the non-trivial symbolic expectation values of the Dirac delta function, and the momentum-dependent orbit–orbit coupling terms are successfully calculated. Results are then used, as an illustration, to compute the semi-relativistic s-wave heavy-light meson masses. We obtain good agreement with experimental data for the meson mass splittings cu¯, cd¯, cs¯, bu¯, bd¯, bs¯.

Highlights

  • The nonexistence of a precise analytical solution to Schrödinger-like wave-equations with different potential models has led the study of such wave-equations to be one of the most common theoretical laboratories for investigating the validity of various methods based on perturbative and non-perturbative approaches

  • PAIM is different from other perturbation approaches [1,6], as it lays no limitations on the coupling constants or the quantum numbers included in the phenomenological potential models

  • We presented a deeply theoretical investigation on the perturbation technique within the framework of the asymptotic iteration method (PAIM)

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Summary

Introduction

The nonexistence of a precise analytical solution to Schrödinger-like wave-equations with different potential models has led the study of such wave-equations to be one of the most common theoretical laboratories for investigating the validity of various methods based on perturbative and non-perturbative approaches. One of the fundamental advantage of PAIM in this respect is that it facilitates choosing a reference Hamiltonian H0 from several available options in H that can be solved exactly within the asymptotic iteration method (AIM) [10,11,12] In this regard, a reasonable problem to tackle the above issue could be the semirelativistic wave-Equation (SR). The transformed SR waveequation is reduced to a form almost the same as the Schrödinger wave-equation with an extra self-induced non-separable energy-dependent harmonic-oscillator field The presence of this term makes the solution to this equation generally more difficult to be solved within the available traditional well-known perturbation techniques [1,15]. We present our summary with concluding remarks on the suggested technique and on its results

Theoretical Framework
K2r4 4
The Explicit Perturbed Symbolic Energy Expressions via PAIM
Conclusions
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