The local well-posedness problem for the Maxwell-Klein-Gordon system in Coulomb gauge as well as Lorenz gauge is treated in two space dimensions for data with minimal regularity assumptions. In the classical case of data in -based Sobolev spaces and for the electromagnetic field and the potential , respectively. The minimal regularity assumptions are $s
\frac{1}{2}l > \frac{1}{4}\frac{1}{2}\frac{1}{4}s_c = l_c =0\widehat{H}^{s,r}\widehat{H}^{l,r}s> \frac{21}{16}l > \frac{9}{8}r1$ , whereas the critical exponents with respect to scaling fulfill , as . Here $|f|{\widehat{H}^{s,r}} := | \langle \xi \rangle^s \tilde{f}|{L^{r’}_{\tau \xi}} , , , 1 < r \le 2 , , , \frac{1}{r}+\frac{1}{r’} = 1 , . \phi$ as well as in both gauges.

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