R. Feynman formulated quantum mechanics in terms of integrals over spaces of paths (Feynman path integrals). But the absolute value of Feynman's integrand is not integrable. And his integrand does not generate a measure. So Lebesgue integration theory could not be used by Feynman. To establish the equivalence of his theory with the traditional formulation of quantum mechanics, Feynman gave an argument that his path integral satisfies Schrödinger's equation. This paper gives a proof of this part of Feynman's theory. To justify Feynman's and other investigators' use of the language and concepts of integration and probability theory, and to justify taking limits under the integral sign in Feynman's integral, we use R. Henstock's approach to non-absolute integration, which does not require the measure concept, and for which the absolute value of the integrand need not be integrable.
Contents
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Requires Authentication UnlicensedFeynman's Path Integrals and Henstock's Non-Absolute IntegrationLicensedJune 4, 2010
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Requires Authentication UnlicensedUniversally Polygonally Approximable FunctionsLicensedJune 4, 2010
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Requires Authentication UnlicensedDifferential Calculus for Complex-Valued MultifunctionsLicensedJune 4, 2010
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Requires Authentication UnlicensedOn Analogues of Some Classical Subsets of the Real LineLicensedJune 4, 2010
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Requires Authentication UnlicensedOscillation Criteria of Comparison Type for Second Order Difference EquationsLicensedJune 4, 2010
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Requires Authentication UnlicensedOn the Convergence of the Method of Lines for Quasi–Nonlinear Functional Evolutions in Banach SpacesLicensedJune 4, 2010
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Requires Authentication UnlicensedBounded Solutions for Nonlinear Elliptic Equations in Unbounded DomainsLicensedJune 4, 2010
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Requires Authentication UnlicensedA Characterization of Strict Local Minimizers of Order One for Static Minmax Problems in the Parametric Constraint CaseLicensedJune 4, 2010
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Requires Authentication UnlicensedOn Linear Dependence of IteratesLicensedJune 4, 2010