  Large scale molecular dynamics simulations are performed to study the steady
state yielding dynamics of a well established simple glass. In contrast to the
supercooled state, where the shear stress, $\sigma$, tends to zero at vanishing
shear rate, $\gammadot$, a stress plateau forms in the glass which extends over
about two decades in shear rate. This strongly suggests the existence of a
finite dynamic yield stress in the glass, $\sigma^+ (T) \equiv \sigma(T;
\gammadot \to 0) >0$. Furthermore, the temperature dependence of $\sigma^+$
suggests a yield stress discontinuity at the glass transition in agreement with
recent theoretical predictions. We scrutinize and support this observation by
testing explicitly for the assumptions (affine flow, absence of flow induced
ordering) inherent in the theory. Also, a qualitative change of the flow curves
enables us to bracket the glass transition temperature $T_c$ of the theory from
above and (for the first time in simulations) {\it from below}. Furthermore,
the structural relaxation time in the steady state behaves quite similar to the
system viscosity at all studied shear rates and temperatures.
