DISCRETE GAUGE-SYMMETRY ANOMALIES

It has been recently argued that quantum gravity effects strongly violate all non-gauge symmetries. This would suggest that all low energy discrete symmetries should be guage symmetries, either continuous or discrete. Acceptable continuous gauge symmetries are constrained by the condition they should be anomaly free. We show here that any discrete gauge symmetry should also obey certain "discrete anomaly cancellation" conditions. These conditions strongly constrain the massless fermion content of the theory and follow from the "parent" cancellation of the usual continuous gauge anomalies. They have interesting applications in model building. As an example we consider the constraints on the Z(N) "generalized matter parities" of the supersymmetric standard model. We show that only a few (including the standard R-parity) are "discrete anomaly free" unless the fermion content of the minimal supersymmetric standard model is enlarged.