Quantum corrections to Lorentz- and CPT-violating QED in flat spacetime
produce unusual radiative corrections, which can be finite but of undetermined
magnitude. The corresponding radiative corrections in a gravitational theory
are even stranger, since the term in the fermion action involving a preferred
axial vector bμ would give rise to a gravitational Chern-Simons term
that is proportional bμ, yet which actually does not break Lorentz
invariance. Initially, the coefficient of this gravitational Chern-Simons term
appears to have the same ambiguity as the coefficient for the analogous term in
QED. However, this puzzle is resolved by the fact that the gravitational theory
has more stringent gauge invariance requirements. Lorentz symmetry in a metric
theory of gravity can only be broken spontaneously, and when the vector
bμ arises from spontaneous symmetry breaking, these specific radiative
corrections are no longer ambiguous but instead must vanish identically.Comment: 16 page