Abstract

We study radiative corrections to massless quantum electrodynamics modified by two dimension-five LV interactions $\bar{\Psi} \gamma^{\mu} b'^{\nu} F_{\mu\nu}\Psi$ and $\bar{\Psi}\gamma^{\mu}b^{\nu} \tilde{F}_{\mu\nu} \Psi$ in the framework of effective field theories. All divergent one-particle-irreducible Feynman diagrams are calculated at one-loop order and several related issues are discussed. It is found that massless quantum electrodynamics modified by the interaction $\bar{\Psi} \gamma^{\mu} b'^{\nu} F_{\mu\nu}\Psi$ alone is one-loop renormalizable and the result can be understood on the grounds of symmetry. In this context the one-loop Lorentz-violating beta function is derived and the corresponding running coefficients are obtained.

Highlights

  • Despite its success to account for most phenomena with precision down to subatomic scales, the standard model of particle physics is incomplete and leaves several issues unsolved

  • The divergent corrections to the photon self-energy are given in Eq [6], and those to the fermion self-energy are given in Eq [8]

  • Our results indicate that other than the usual quantum electrodynamics (QED) divergences, all new divergent corrections are due to the LV operatorγ μbν Fμν

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Summary

Introduction

Despite its success to account for most phenomena with precision down to subatomic scales, the standard model of particle physics is incomplete and leaves several issues unsolved. One possible resolution is that the currently unknown underlying theory prohibits the generation of the renormalizable LV operators at low energies. Probing this scenario at highenergy scales would be interesting but lies beyond the scope of this paper. This conception raises the interest in studying the LV terms of nonrenormalizable dimensions. Even in the simplified case where massless QED is modified by the two non-minimal LV operators mentioned above, a comprehensive study of one-loop radiative corrections to this model is still lacking.

One-loop corrections
Photon self-energy
Fermion self-energy
Three-point fermion-photon vertex
Four-point fermion-photon vertex
Conclusion

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