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Communications in Mathematical Physics

On the Feynman Path Integral for the Dirac Equation in the General Dimensional Spacetime

Wataru Ichinose

Published Mar 20, 2014• 9 citations
Publisher
DOI
10.1007/s00220-014-1997-x

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The Feynman path integral plays a central role in quantum mechanics, linking classical action to propagators and relating quantum electrodynamics (QED) to Feynman diagrams. However, the path-integral formulations used in non-relativistic quantum mechanics and in QED are neither unified nor directly connected. This suggests the existence of a missing path integral that bridges relativistic action and the Dirac equation at the single-particle level. In this work, we analyze the consistency and completeness of existing path-integral theories and identify a spinor path integral that fills this gap. Starting from a relativistic action written in spinor form, we construct a spacetime path integral whose kernel reproduces the Dirac Hamiltonian. The resulting formulation provides a direct link between the relativistic classical action and the Dirac equation, and it naturally extends the scalar relativistic path integral developed in our earlier work. Beyond establishing this structural connection, the spinor path integral offers a new way to interpret the origin of classical mechanics for the Dirac equation and suggests a spacetime mechanism for spin and quantum nonlocal correlations. These features indicate that the spinor path integral can serve as a unifying framework for existing path-integral approaches and as a starting point for further investigations into the spacetime structure of quantum mechanics.
We review the algorithm of Feit, Fleck and Steiger [1] as a method to calculate Feynman Path integrals in real time under very general circumstances ranging from the simple potential problems for the Schroedinger equation to cases involving time dependent perturbations, resonances and coupling to a white noise source. Dirac equation can be studied with minor modifications. We test the algorithm in the one-dimensional Dirac equation using the potential tanh (λ x ) which allows for an exact solution.