2022
DOI: 10.1142/s0219887823500603
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Topological defects with generalized Hulthen–Coulomb-inverse quadratic Yukawa potential on eigenvalue solution under Aharonov–Bohm flux field

Abstract: In this work, we solve the radial Schrödinger wave equation in three dimensions under Aharonov–Bohm (AB)-flux field with potential superposition of generalized q-deformed Hulthen potential, Coulomb potential, and inverse quadratic Yukawa potential in a point-like defect. We determine the approximate eigenvalue solution using the parametric Nikiforov–Uvarov (NU) method and analyze the effects of topological defect and the magnetic flux field with this superposed potential. We show an analogous of the AB effect … Show more

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Cited by 14 publications
(9 citation statements)
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“…The time-dependent Schrödinger wave equation with potential V(r) and electromagnetic potential  A is described by the following wave equation [9][10][11][12][13][14][15][16][17] [7, 11, 15-17, 28, 29], i = 1, 2, 3 and e is the electric charges. For the space-time geometry (1) under consideration, its (spatial part) determinant is given by = = q a g g ij r sin…”
Section: Schrödinger Non-relativistic Particles Confined By Ab-flux I...mentioning
confidence: 99%
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“…The time-dependent Schrödinger wave equation with potential V(r) and electromagnetic potential  A is described by the following wave equation [9][10][11][12][13][14][15][16][17] [7, 11, 15-17, 28, 29], i = 1, 2, 3 and e is the electric charges. For the space-time geometry (1) under consideration, its (spatial part) determinant is given by = = q a g g ij r sin…”
Section: Schrödinger Non-relativistic Particles Confined By Ab-flux I...mentioning
confidence: 99%
“…However, the non-relativistic Schrodinger wave equation with some potential models in the background of a point-like global monopole spacetime has been investigated in a few works. These works include a harmonic oscillator [9], a harmonic oscillator with potential (linear, Coulomb and Cornell-type) [10], a harmonic oscillator with Mie-type potential under the AB-flux field [11], scattering of charged particles by an Abelian magnetic monopole [12], non-relativistic particles interact with potential, such as Kratzer and Morse potential [13], generalized Morse potential [14], a diatomic molecular potential [15], pseudoharmonic-and Mie-type potentials [16], and generalized q-deformed Hulthen plus Coulomb and inverse quadratic Yukawa potential [17].…”
Section: Introductionmentioning
confidence: 99%
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