Unveiling the role of vector potential in the Aharonov-Bohm effect

TL;DR

This paper argues that the vector potential in the Aharonov-Bohm effect has a physically meaningful, gauge-invariant component that fundamentally explains the observed phase shift, challenging the view that it is merely a mathematical tool.

Contribution

The paper provides convincing arguments that the vector potential contains a unique, gauge-invariant part responsible for the AB phase shift, emphasizing its physical significance.

Findings

Identifies a gauge-invariant component of the vector potential responsible for the AB effect.

Argues that the vector potential's physical effects cannot be fully eliminated by gauge transformations.

Supports the view that the vector potential has a fundamental physical role in quantum phenomena.

Abstract

The most popular interpretation of the Aharonov-Bohm (AB) effect is that the electromagnetic potential locally affects the complex phase of a charged particle's wave function in the magnetic field free region. However, since the vector potential is a gauge-variant quantity, not a few researchers suspect that it is just a convenient tool for calculating the force field. This motivates them to explain the AB effect without using the vector potential, which inevitably leads to some sort of non-locality. This frustrating situation is shortly summarized by the statement of Aharonov et al. that the AB effect may be due to a local gauge potential or due to non-local gauge-invariant fields. In the present paper, we shall give several convincing arguments, which support the viewpoint that the vector potential is not just a convenient mathematical tool with little physical entity. Despite its gauge arbitrariness, the vector potential certainly contains a gauge-invariant piece, which solely explains the observed AB phase shift. Importantly, this component has a property such that it is basically unique and cannot be eliminated by any regular gauge transformations. To make the discussion complete, we also discuss the role of remaining gauge arbitrariness still contained in the entire vector potential.