“…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.…”