A physically-motivated quantisation of the electromagnetic field

TL;DR

This paper presents a physically-motivated approach to quantising the electromagnetic field directly from experimental observations, avoiding traditional gauge and boundary condition assumptions used in standard methods.

Contribution

It introduces a novel quantisation method based on observable fields, bypassing the need for vector potentials and artificial boundary conditions.

Findings

Electric and magnetic field observables follow from Heisenberg's equations

The approach does not require gauge fixing or cavity boundary conditions

Provides a more physically intuitive quantisation framework

Abstract

The notion that the electromagnetic field is quantised is usually inferred from observations such as the photoelectric effect and the black-body spectrum. However accounts of the quantisation of this field are usually mathematically motivated and begin by introducing a vector potential, followed by the imposition of a gauge that allows the manipulation of the solutions of Maxwell's equations into a form that is amenable for the machinery of canonical quantisation. By contrast, here we quantise the electromagnetic field in a less mathematically and more physically-motivated way. Starting from a direct description of what one sees in experiments, we show that the usual expressions of the electric and magnetic field observables follow from Heisenberg's equation of motion. In our treatment, there is no need to invoke the vector potential in a specific gauge and we avoid the commonly-used notion of a fictitious cavity that applies boundary conditions to the field.