Quantum mechanics without potential function
Abstract
In the standard formulation of quantum mechanics, one starts by proposing a potential function that models the physical system. The potential is then inserted into the Schrödinger equation, which is solved for the wavefunction, bound states energy spectrum, and/or scattering phase shift. In this work, however, we propose an alternative formulation in which the potential function does not appear. The aim is to obtain a set of analytically realizable systems, which is larger than in the standard formulation and may or may not be associated with any given or previously known potential functions. We start with the wavefunction, which is written as a bounded infinite sum of elements of a complete basis with polynomial coefficients that are orthogonal on an appropriate domain in the energy space. Using the asymptotic properties of these polynomials, we obtain the scattering phase shift, bound states, and resonances. This formulation enables one to handle not only the well-known quantum systems but also previously untreated ones. Illustrative examples are given for two- and three-parameter systems.
- Authors:
-
- Department of Mathematics, University of Central Florida, Orlando, Florida 32816 (United States)
- Publication Date:
- OSTI Identifier:
- 22479578
- Resource Type:
- Journal Article
- Journal Name:
- Journal of Mathematical Physics
- Additional Journal Information:
- Journal Volume: 56; Journal Issue: 7; Other Information: (c) 2015 AIP Publishing LLC; Country of input: International Atomic Energy Agency (IAEA); Journal ID: ISSN 0022-2488
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; ASYMPTOTIC SOLUTIONS; BOUND STATE; ENERGY SPECTRA; PHASE SHIFT; POLYNOMIALS; POTENTIALS; QUANTUM MECHANICS; QUANTUM SYSTEMS; SCATTERING; SCHROEDINGER EQUATION; SPACE; WAVE FUNCTIONS
Citation Formats
Alhaidari, A. D., E-mail: haidari@sctp.org.sa, and Ismail, M. E. H. Quantum mechanics without potential function. United States: N. p., 2015.
Web. doi:10.1063/1.4927262.
Alhaidari, A. D., E-mail: haidari@sctp.org.sa, & Ismail, M. E. H. Quantum mechanics without potential function. United States. https://doi.org/10.1063/1.4927262
Alhaidari, A. D., E-mail: haidari@sctp.org.sa, and Ismail, M. E. H. 2015.
"Quantum mechanics without potential function". United States. https://doi.org/10.1063/1.4927262.
@article{osti_22479578,
title = {Quantum mechanics without potential function},
author = {Alhaidari, A. D., E-mail: haidari@sctp.org.sa and Ismail, M. E. H.},
abstractNote = {In the standard formulation of quantum mechanics, one starts by proposing a potential function that models the physical system. The potential is then inserted into the Schrödinger equation, which is solved for the wavefunction, bound states energy spectrum, and/or scattering phase shift. In this work, however, we propose an alternative formulation in which the potential function does not appear. The aim is to obtain a set of analytically realizable systems, which is larger than in the standard formulation and may or may not be associated with any given or previously known potential functions. We start with the wavefunction, which is written as a bounded infinite sum of elements of a complete basis with polynomial coefficients that are orthogonal on an appropriate domain in the energy space. Using the asymptotic properties of these polynomials, we obtain the scattering phase shift, bound states, and resonances. This formulation enables one to handle not only the well-known quantum systems but also previously untreated ones. Illustrative examples are given for two- and three-parameter systems.},
doi = {10.1063/1.4927262},
url = {https://www.osti.gov/biblio/22479578},
journal = {Journal of Mathematical Physics},
issn = {0022-2488},
number = 7,
volume = 56,
place = {United States},
year = {Wed Jul 15 00:00:00 EDT 2015},
month = {Wed Jul 15 00:00:00 EDT 2015}
}