Abstract

Non-relativistic quantum mechanics is formulated here in a different way. It is, however, mathematically equivalent to the familiar formulation. In quantum mechanics the probability of an event which can happen in several different ways is the absolute square of a sum of complex contributions, one from each alternative way. The probability that a particle will be found to have a path x(t) lying somewhere within a region of space time is the square of a sum of contributions, one from each path in the region. The contribution from a single path is postulated to be an exponential whose (imaginary) phase is the classical action (in units of ℏ) for the path in question. The total contribution from all paths reaching x, t from the past is the wave function ψ(x, t). This is shown to satisfy Schroedinger's equation. The relation to matrix and operator algebra is discussed. Applications are indicated, in particular to eliminate the coordinates of the field oscillators from the equations of quantum electrodynamics.

Keywords

PhysicsPath integral formulationAction (physics)Quantum mechanicsRelativistic quantum mechanicsSchrödinger equationRelation between Schrödinger's equation and the path integral formulation of quantum mechanicsOperator (biology)Phase spaceQuantumClassical mechanicsWave functionMathematical physicsQuantum dissipation

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Publication Info

Year
1948
Type
article
Volume
20
Issue
2
Pages
367-387
Citations
4118
Access
Closed

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Richard P. Feynman (1948). Space-Time Approach to Non-Relativistic Quantum Mechanics. Reviews of Modern Physics , 20 (2) , 367-387. https://doi.org/10.1103/revmodphys.20.367

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DOI
10.1103/revmodphys.20.367