2010
DOI: 10.1142/s0217751x10049293
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Bare and Induced Lorentz and CPT Invariance Violations in Qed

Abstract: We consider QED in a constant axial vector background (AEther). Further Lorentz invariance violations (LIV) might occur owing to radiative corrections. The phenomenology of this model is studied, clarifying issues related to the various regularizations employed, with a particular emphasis on the induced photon mass. To this concern, it is shown that in the presence of LIV dimensional regularization may produce a radiatively induced finite photon mass. The possible physical role of the large momentum cutoff is … Show more

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Cited by 97 publications
(57 citation statements)
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References 105 publications
(164 reference statements)
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“…The appearance of this term in the energy density can introduce instability in the theory [21,22], and it can be resolved by requiring that only spacelike components of k μ are nonzero. However, this condition depends on the observer frame, so even an infinitesimal boost to another observer frame would reintroduce instability.…”
Section: Lorentz-violating Electrodynamicsmentioning
confidence: 99%
“…The appearance of this term in the energy density can introduce instability in the theory [21,22], and it can be resolved by requiring that only spacelike components of k μ are nonzero. However, this condition depends on the observer frame, so even an infinitesimal boost to another observer frame would reintroduce instability.…”
Section: Lorentz-violating Electrodynamicsmentioning
confidence: 99%
“…The general solutions of the equations for the Maxwell-Chern-Simons free quantum field, have been extensively discussed and applied in [72,73] for the massive case and in [14] for the massless case. However, in the light of the present applications it's better to shortly overview this topic.…”
Section: The Chern-simons Limit For the Pseudoscalar Backgroundmentioning
confidence: 99%
“…Here we aim to develop a rather general frame which could allow to readily interplay among the massive, massless, temporal and spatial cases, as we shall specify in the sequel. The starting point is the rank-two symmetric matrix [72] …”
Section: Canonical Quantization Of the Maxwell-chern-simons Fieldmentioning
confidence: 99%
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