The Relativistic Hamilton-Jacobi Equation for a Massive, Charged and Spinning Particle, its Equivalent Dirac Equation and the de Broglie-Bohm Theory
Wadyr A. Rodrigues Jr., Samuel A. Wainer

TL;DR
This paper demonstrates the equivalence between the classical relativistic Hamilton-Jacobi equation for a spinning, charged particle and a Dirac-Hestenes equation, revealing insights into quantum potential constraints and experimental discrepancies in de Broglie-Bohm theory.
Contribution
It establishes a novel equivalence between classical relativistic Hamilton-Jacobi and Dirac-Hestenes equations for spinning particles using Clifford formalisms.
Findings
Classical Hamilton-Jacobi equation is equivalent to a Dirac-Hestenes equation for certain spinor fields.
The quantum potential in the generalized Hamilton-Jacobi equation is subject to a severe constraint.
The particle's mass becomes a variable in the generalized Dirac-Hestenes equation.
Abstract
Using the Clifford and the Spin-Clifford formalisms we prove that the classical relativistic Hamilton Jacobi equation for a charged massive (and spinning) particle interacting with an external electromagnetic field is equivalent to a Dirac-Hestenes equation satisfied by a class of spinor fields that we call classical spinor fields, characterized for having the Takabayashi angle function constant (equal to 0 or {\pi}). We also investigate a nonlinear Dirac-Hestenes like equation that comes from some class of generalized classical spinor fields. Finally we show that the general Dirac-Hestenes equation (which is a representative in the Clifford bundle of the usual Dirac equation) gives a generalized Hamilton-Jacobi equation where the quantum potential satisfy a severe constraint and the "mass of the particle" becomes a variable. Our results can then explain the experimental discrepancies…
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