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
Summary
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.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.