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Schrödinger Equation Solutions for the Central Field Power Potential Energy II. V(r) = −V 0(r/a 0)2ν−2, 0 ≤ ν ≤ 1, the Bound States

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Abstract

The bound states of the generalized Schrödinger equation system with radial potential energy V(r) = −V 0(r/a 0)2ν−2, 0 ≤ ν ≤ 1, are described. The solutions of the differential equation are related to the functions for the bound state problem with ν ≥ 1. The Green's function is constructed as well as its first iteration, the traces of both functions are calculated, and an upper and lower bound for the ground state is established. A WKB-like approximate solution for the eigenvalues and eigenfunctions is derived.

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References

  1. P.C. McKinney, Schrödinger equation solutions for the central field power potential energy, I. V(r) = V0(r/a0)2v-2,v ⩾ 1, J. Math. Chem. 32(4) (2002) 381-404 (this issue).

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McKinney, P.C. Schrödinger Equation Solutions for the Central Field Power Potential Energy II. V(r) = −V 0(r/a 0)2ν−2, 0 ≤ ν ≤ 1, the Bound States. Journal of Mathematical Chemistry 32, 405–410 (2002). https://doi.org/10.1023/A:1022957623388

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  • DOI: https://doi.org/10.1023/A:1022957623388

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