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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Bibliographic Details
Main Author: Hefley, Velton Wade
Other Authors: Kobe, Donald Holm
Format: Others
Language:English
Published: North Texas State University 1977
Subjects:
Online Access:https://digital.library.unt.edu/ark:/67531/metadc504591/
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spelling 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.
collection NDLTD
language English
format Others
sources NDLTD
topic quantum theory
space-time
Schrödinger equation
Newtonian mechanics
Mechanics.
Quantum theory.
Feynman integrals.
Ehrenfest theorem.
spellingShingle 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/
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