The behaviour of scalar electrodynamics under symmetry breaking by the
Higgs mechanism is studied in a class of dynamical spacetimes-those h
aving a Bianchi type I symmetry-which includes the spatially flat Robe
rtson-Walker spacetimes. The Einstein equations are used to obtain the
effective Lagrangian, from which it is shown that either the gauge fi
eld does not become massive during symmetry breaking (in marked contra
st with the case in which the background spacetime is static), or the
symmetry breaking chooses not only a direction in the phase space of t
he Higgs field, but also a spatial direction in the spacetime sections
.