The Classical Limit of Quantum Mechanics
The Feynman path integral formulation of quantum mechanics is a path integral representation for a propagator or probability amplitude in going between two points in space-time. The wave function is expressed in terms of an integral equation from which the Schrodinger equation can be derived. On tak...
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1977
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ndltd-unt.edu-info-ark-67531-metadc5045912017-03-17T08:41:25Z The Classical Limit of Quantum Mechanics Hefley, Velton Wade quantum theory space-time Schrödinger equation Newtonian mechanics Mechanics. Quantum theory. Feynman integrals. Ehrenfest theorem. The Feynman path integral formulation of quantum mechanics is a path integral representation for a propagator or probability amplitude in going between two points in space-time. The wave function is expressed in terms of an integral equation from which the Schrodinger equation can be derived. On taking the limit h — 0, the method of stationary phase can be applied and Newton's second law of motion is obtained. Also, the condition the phase vanishes leads to the Hamilton - Jacobi equation. The secondary objective of this paper is to study ways of relating quantum mechanics and classical mechanics. The Ehrenfest theorem is applied to a particle in an electromagnetic field. Expressions are found which are the hermitian Lorentz force operator, the hermitian torque operator, and the hermitian power operator. North Texas State University Kobe, Donald Holm Basbas, George J. 1977-12 Thesis or Dissertation v, 89 leaves : graphs Text local-cont-no: 1002772813-Hefley call-no: 379 N81 no.5431 untcat: b1135393 oclc: 3917641 https://digital.library.unt.edu/ark:/67531/metadc504591/ ark: ark:/67531/metadc504591 English Public Hefley, Velton Wade Copyright Copyright is held by the author, unless otherwise noted. All rights reserved. |
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English |
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Others
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quantum theory space-time Schrödinger equation Newtonian mechanics Mechanics. Quantum theory. Feynman integrals. Ehrenfest theorem. |
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quantum theory space-time Schrödinger equation Newtonian mechanics Mechanics. Quantum theory. Feynman integrals. Ehrenfest theorem. Hefley, Velton Wade The Classical Limit of Quantum Mechanics |
description |
The Feynman path integral formulation of quantum mechanics is a path integral representation for a propagator or probability amplitude in going between two points in space-time. The wave function is expressed in terms of an integral equation from which the Schrodinger equation can be derived. On taking the limit h — 0, the method of stationary phase can be applied and Newton's second law of motion is obtained. Also, the condition the phase vanishes leads to the Hamilton - Jacobi equation. The secondary objective of this paper is to study ways of relating quantum mechanics and classical mechanics. The Ehrenfest theorem is applied to a particle in an electromagnetic field. Expressions are found which are the hermitian Lorentz force operator, the hermitian torque operator, and the hermitian power operator. |
author2 |
Kobe, Donald Holm |
author_facet |
Kobe, Donald Holm Hefley, Velton Wade |
author |
Hefley, Velton Wade |
author_sort |
Hefley, Velton Wade |
title |
The Classical Limit of Quantum Mechanics |
title_short |
The Classical Limit of Quantum Mechanics |
title_full |
The Classical Limit of Quantum Mechanics |
title_fullStr |
The Classical Limit of Quantum Mechanics |
title_full_unstemmed |
The Classical Limit of Quantum Mechanics |
title_sort |
classical limit of quantum mechanics |
publisher |
North Texas State University |
publishDate |
1977 |
url |
https://digital.library.unt.edu/ark:/67531/metadc504591/ |
work_keys_str_mv |
AT hefleyveltonwade theclassicallimitofquantummechanics AT hefleyveltonwade classicallimitofquantummechanics |
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1718432547950559232 |