Table of Contents
Fetching ...

Maxwell theories along the light track: Null Formalism in extended electrodynamics

Zhi Xiao, Bing Sun, Tao Zhu

Abstract

We develop a differential-form approach to systematically derive the Newman-Penrose null-tetrad equations for Lorentz-violating extensions of Maxwell electrodynamics. The coordinate-independent nature of differential forms allows the actions and corresponding field equations of the theory to be expressed compactly and enables a systematic and transparent derivation of first-order equations in the Newman-Penrose formalism. Within this formalism, we explicitly present a simple algebraic construction for the gauge invariant extended Maxwell actions that avoids explicit index manipulations up to mass dimension six. The combined scheme of differential-form approach and Newman-Penrose formalism offers an efficient tool for analyzing Lorentz-violating effects on asymptotic photon propagation and polarization.

Maxwell theories along the light track: Null Formalism in extended electrodynamics

Abstract

We develop a differential-form approach to systematically derive the Newman-Penrose null-tetrad equations for Lorentz-violating extensions of Maxwell electrodynamics. The coordinate-independent nature of differential forms allows the actions and corresponding field equations of the theory to be expressed compactly and enables a systematic and transparent derivation of first-order equations in the Newman-Penrose formalism. Within this formalism, we explicitly present a simple algebraic construction for the gauge invariant extended Maxwell actions that avoids explicit index manipulations up to mass dimension six. The combined scheme of differential-form approach and Newman-Penrose formalism offers an efficient tool for analyzing Lorentz-violating effects on asymptotic photon propagation and polarization.
Paper Structure (13 sections, 88 equations, 1 figure, 1 table)

This paper contains 13 sections, 88 equations, 1 figure, 1 table.

Figures (1)

  • Figure 1: Rays in a linearized radiation field. Figure is copied from the Ref. Sachs1960s. In this figure, $k^a$ is denoted as the first null vector $l^\mu$, $v(x)$ is the affine parameter $r$, and $z^a[r^s(x)]$ is the source world line with four-velocity $e^a=dz^a/ds$.