We discuss the chirally symmetric solution of the massless, quenched,
Dyson-Schwinger equation for the fermion propagator in three and four
dimensions. The solutions are manifestly gauge covariant. We consider
a gauge covariance constraint on the fermion-gauge-boson vertex, which
motivates a vertex Ansatz that both satisfies the Ward identity when
the fermion self-mass is zero and ensures gauge covariance of the ferm
ion propagator.