2009
DOI: 10.1140/epjd/e2009-00096-6
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Exact solution of N-dimensional radial Schrödinger equation for the fourth-order inverse-power potential

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Cited by 19 publications
(17 citation statements)
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“…With the help of equations (32) and (33a)-(33e), the expansion coefficients a n in equation (35) satisfy the following recursion relation [72] a n+1 = 4λ 2 −9−4(n+λ+2) 2(n+λ+2) 2 a n−1 .…”
Section: 、Generalized Dirac Oscillator With a Topological Defectmentioning
confidence: 99%
“…With the help of equations (32) and (33a)-(33e), the expansion coefficients a n in equation (35) satisfy the following recursion relation [72] a n+1 = 4λ 2 −9−4(n+λ+2) 2(n+λ+2) 2 a n−1 .…”
Section: 、Generalized Dirac Oscillator With a Topological Defectmentioning
confidence: 99%
“…The surface element in D spatial dimension is DC D r D−1 dr, where the explicit expression of the terms C D has been stated in section 2.1. As the wave function in this case contains Airy's infinite polynomial series, we calculate < H > through numerical integration using the following integrals: (27) In this case, with Airy's function involved in the wave function, simpler equations like (13)(14)(15)(16)(17)(18)(19)(20)(21)(22) in the large D limit are not possible as we follow numerical integration to evaluate terms < H 1 >, < H 2 >, < H 3 >.…”
Section: Mass With Linear Term As Parentmentioning
confidence: 99%
“…In the recent B Damian Mikulski dmkwant@amu.edu.pl 1 years authors have analytically derived exact solutions for diverse potentials, i.a. the fourth-order inverse power potential [1][2][3]:…”
Section: Introductionmentioning
confidence: 99%