1995
DOI: 10.1103/physrevd.51.5961
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Lorentz symmetry breaking in Abelian vector-field models with Wess-Zumino interaction

Abstract: We consider the abelian vector-field models in the presence of the Wess-Zumino interaction with the pseudoscalar matter. The occurence of the dynamic breaking of Lorentz symmetry at classical and one-loop level is described for massless and massive vector fields. This phenomenon appears to be the non-perturbative counterpart of the perturbative renormalizability and/or unitarity breaking in the chiral gauge theories. a

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Cited by 94 publications
(85 citation statements)
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References 20 publications
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“…The possibility of a vacuum that breaks LI and has non-trivial optical properties has already been investigated in [29,30]. This work, however, deals with significantly more complicated models, both in terms of the interactions that spontaneously break LI and of the optical properties of the resulting vacuum.…”
Section: Phenomenology Of Lorentz Violation By a Background Sourcementioning
confidence: 99%
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“…The possibility of a vacuum that breaks LI and has non-trivial optical properties has already been investigated in [29,30]. This work, however, deals with significantly more complicated models, both in terms of the interactions that spontaneously break LI and of the optical properties of the resulting vacuum.…”
Section: Phenomenology Of Lorentz Violation By a Background Sourcementioning
confidence: 99%
“…(30) gives it a finite time-like VEV, which would imply a finite VEV forψγ µ ψ in the theory of Eq. (29). We argued in the previous section that g must be large for the theory described by Eq.…”
Section: Consequences For Emergent Photonsmentioning
confidence: 99%
“…In the case of the fields A 1 µ and A 2 µ , the propagator was studied in the reference [26]. The conclusions on the c µ vector were the same as in [3], [8], [11]: it must be spacelike. So, the quantization of our non-Abelian theory can be carried out without problems provided that c µ is spacelike.…”
Section: Concluding Commentsmentioning
confidence: 99%
“…We thus find two kinds of propagators, when spontaneous symmetry breaking takes place: one for the massless field A 3 µ , which is in the internal direction of the U(1) remnant symmetry, and another for the massive, A 1 µ and A 2 µ , fields. The quantization consistency for a theory with the propagator for the massless A 3 µ -field was analyzed in the paper [3], [8], [11]. In these work, aspects like unitarity and microcausality were considered and the unique possibility of a consistent theory is the one in which the external vector, c µ , is spacelike.…”
Section: Concluding Commentsmentioning
confidence: 99%
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