Lorentz Covariant Quantum 4-Potential and Orbital Angular Momentum for the Transverse Confinement of Matter Waves

TL;DR

This paper introduces a Lorentz covariant quantum 4-potential linked to transverse confinement in matter waves, clarifies the role of canonical and kinetic momenta, and shows OAM as a manifestation of this potential in relativistic quantum mechanics.

Contribution

It defines a Lorentz covariant quantum 4-potential for matter waves and demonstrates its role in orbital angular momentum, advancing understanding of relativistic transverse confinement.

Findings

Quantum 4-potential couples into canonical 4-momentum.

Kinetic 4-momentum does not contribute to OAM.

OAM is a pure manifestation of the quantum 4-potential.

Abstract

In two recent papers exact Hermite-Gaussian solutions to relativistic wave equations have been obtained for both electromagnetic and particle beams that include Gouy phase. The solutions for particle beams correspond to those of the Schr\"{o}dinger equation in the non-relativistic limit. Here, distinct canonical and kinetic 4-momentum operators will be defined for quantum particles in matter wave beams. The kinetic momentum is equal to the canonical momentum minus the fluctuating terms resulting from the transverse localization of the beam. Three results are obtained. First, the total energy of a particle for each beam mode is calculated. Second, the localization terms couple into the canonical 4-momentum of the beam particles as a Lorentz covariant quantum 4-potential originating at the waist. The quantum 4-potential plays an analogous role in relativistic Hamiltonian quantum mechanics to the Bohm potential in the non-relativistic quantum Hamilton-Jacobi equation. Third, the orbital angular momentum (OAM) operator must be defined in terms of canonical momentum operators. It is further shown that kinetic 4-momentum does not contribute to OAM indicating that OAM can therefore be regarded as a pure manifestation of quantum 4-potential.