The Third Five-Parametric Hypergeometric Quantum-Mechanical Potential

We introduce the third five-parametric ordinary hypergeometric energy-independent quantum-mechanical potential, after the Eckart and Pöschl-Teller potentials, which is proportional to an arbitrary variable parameter and has a shape that is independent of that parameter. Depending on an involved para...

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Main Authors: T. A. Ishkhanyan, A. M. Ishkhanyan
Format: Article
Language:English
Published: Wiley 2018-01-01
Series:Advances in High Energy Physics
Online Access:http://dx.doi.org/10.1155/2018/2769597
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author T. A. Ishkhanyan
A. M. Ishkhanyan
author_facet T. A. Ishkhanyan
A. M. Ishkhanyan
author_sort T. A. Ishkhanyan
collection DOAJ
description We introduce the third five-parametric ordinary hypergeometric energy-independent quantum-mechanical potential, after the Eckart and Pöschl-Teller potentials, which is proportional to an arbitrary variable parameter and has a shape that is independent of that parameter. Depending on an involved parameter, the potential presents either a short-range singular well (which behaves as inverse square root at the origin and vanishes exponentially at infinity) or a smooth asymmetric step-barrier (with variable height and steepness). The general solution of the Schrödinger equation for this potential, which is a member of a general Heun family of potentials, is written through fundamental solutions each of which presents an irreducible linear combination of two Gauss ordinary hypergeometric functions.
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spelling doaj-art-0d55c62190334616be12a92c9dd44a742025-02-03T01:02:45ZengWileyAdvances in High Energy Physics1687-73571687-73652018-01-01201810.1155/2018/27695972769597The Third Five-Parametric Hypergeometric Quantum-Mechanical PotentialT. A. Ishkhanyan0A. M. Ishkhanyan1Russian-Armenian University, Yerevan 0051, ArmeniaRussian-Armenian University, Yerevan 0051, ArmeniaWe introduce the third five-parametric ordinary hypergeometric energy-independent quantum-mechanical potential, after the Eckart and Pöschl-Teller potentials, which is proportional to an arbitrary variable parameter and has a shape that is independent of that parameter. Depending on an involved parameter, the potential presents either a short-range singular well (which behaves as inverse square root at the origin and vanishes exponentially at infinity) or a smooth asymmetric step-barrier (with variable height and steepness). The general solution of the Schrödinger equation for this potential, which is a member of a general Heun family of potentials, is written through fundamental solutions each of which presents an irreducible linear combination of two Gauss ordinary hypergeometric functions.http://dx.doi.org/10.1155/2018/2769597
spellingShingle T. A. Ishkhanyan
A. M. Ishkhanyan
The Third Five-Parametric Hypergeometric Quantum-Mechanical Potential
Advances in High Energy Physics
title The Third Five-Parametric Hypergeometric Quantum-Mechanical Potential
title_full The Third Five-Parametric Hypergeometric Quantum-Mechanical Potential
title_fullStr The Third Five-Parametric Hypergeometric Quantum-Mechanical Potential
title_full_unstemmed The Third Five-Parametric Hypergeometric Quantum-Mechanical Potential
title_short The Third Five-Parametric Hypergeometric Quantum-Mechanical Potential
title_sort third five parametric hypergeometric quantum mechanical potential
url http://dx.doi.org/10.1155/2018/2769597
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