Table of Contents
Fetching ...

Photon Quantum Mechanics

Margaret Hawton

TL;DR

Addresses the problem of localizing photons by promoting EM fields to a covariant quantum theory via second quantization in the Lorenz gauge. It derives a real, normalized single-photon density $ρ_p(x)$ with $∫ ρ_p(x) d^3x = 1$ and defines Schrödinger-like operators for position, momentum, energy, and angular momentum. The approach yields a consistent photon current and four-momentum densities in a manifestly covariant framework and clarifies the role of positive and negative frequencies. This work provides a practical, CPT-consistent route to single-photon quantum mechanics suitable for first-pass context in AI and search tooling.

Abstract

We second quantize the standard electromagnetic Lagrangian with a subsiduary Lorenz gauge constraint to obtain a covariant theory of the discrete excitations of the classical EM field that can properly be called photons. The longitudinal photon number is zero due to cancellation of Gupta-Bleuler like terms. Physical photons are described by a real number density whose spatial integral is unity so it can be interpreted as the probability density to find a photon at position x'. Energy density is not separated into is positive and negative frequency parts so the nonlocal frequency operator is not required.

Photon Quantum Mechanics

TL;DR

Addresses the problem of localizing photons by promoting EM fields to a covariant quantum theory via second quantization in the Lorenz gauge. It derives a real, normalized single-photon density with and defines Schrödinger-like operators for position, momentum, energy, and angular momentum. The approach yields a consistent photon current and four-momentum densities in a manifestly covariant framework and clarifies the role of positive and negative frequencies. This work provides a practical, CPT-consistent route to single-photon quantum mechanics suitable for first-pass context in AI and search tooling.

Abstract

We second quantize the standard electromagnetic Lagrangian with a subsiduary Lorenz gauge constraint to obtain a covariant theory of the discrete excitations of the classical EM field that can properly be called photons. The longitudinal photon number is zero due to cancellation of Gupta-Bleuler like terms. Physical photons are described by a real number density whose spatial integral is unity so it can be interpreted as the probability density to find a photon at position x'. Energy density is not separated into is positive and negative frequency parts so the nonlocal frequency operator is not required.
Paper Structure (3 sections, 31 equations)

This paper contains 3 sections, 31 equations.