  We consider the low regularity well-posedness problem for the Maxwell-Dirac
system in n+1 dimensions in the cases $n=3$ and $n=2$ : \begin{align*}
\partial^{\mu} F_{\mu \nu} & = - \langle \psi,\alpha_{\nu} \psi \rangle \\ -i
\alpha^{\mu} \partial_{\mu} \psi & = A_{\mu} \alpha^{\mu} \psi \, ,
\end{align*} where $ F_{\mu \nu} = \partial^{\mu} A_{\nu} - \partial^{\nu}
A_{\mu}$ , and $\alpha^{\mu}$ are the Dirac matrices. We assume the temporal
gauge $A_0=0$ and make use of the fact that some of the nonlinearities fulfill
a null condition. Because we work in the temporal gauge we also apply a method,
which was used by Tao for the Yang-Mills system in this gauge.
