Abstract

In this work we focus on the Carroll-Field-Jackiw (CFJ) modified electrodynamics in combination with a CPT-even Lorentz-violating contribution. We add a photon mass term to the Lagrange density and study the question whether this contribution can render the theory unitary at tree-level. The analysis is based on the pole structure of the modified photon propagator as well as the validity of the optical theorem. We find, indeed, that the massive CFJ-type modification is unitary at tree-level. This result provides a further example for how a photon mass can mitigate malign behaviors.

Highlights

  • Lorentz symmetry violation has been of permanent interest in the past two decades whereby the major part of the investigations have been carried out within the minimal Standard-Model Extension (SME) [1, 2]

  • There has been a vast interest in understanding the properties of the CPT-odd photon sector of the SME that is represented by the Carroll-Field-Jackiw (CFJ) electrodynamics [9]

  • This theory has been extensively examined in the literature with respect to its consistency [10], modifications that it induces in quantum electrodynamics (QED) [11, 12], its radiative generation [13], and many other aspects

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Summary

Introduction

Lorentz symmetry violation has been of permanent interest in the past two decades whereby the major part of the investigations have been carried out within the minimal Standard-Model Extension (SME) [1, 2]. There has been a vast interest in understanding the properties of the CPT-odd photon sector of the SME that is represented by the Carroll-Field-Jackiw (CFJ) electrodynamics [9]. Adding a mass to the graviton renders gravity renormalizable (despite being plagued by the Boulware-Deser ghost [14] that is removed by the construction of de Rham, Gabadadze, and Tolley [15]) It was indicated in [1] and demonstrated in [16] that a photon mass is capable of mitigating the malign behavior in CFJ electrodynamics.

Theoretical setting
Polarization vectors
Application to electroweak sector
Conclusions

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