Inverse scattering at fixed energy for radial magnetic Schr{\"o}dinger operators with obstacle in dimension two

We study an inverse scattering problem at fixed energy for radial magnetic Schr{"o}dinger operators on R^2 \ B(0, r_0), where r_0 is a positive and arbitrarily small radius. We assume that the magnetic potential A satisfies a gauge condition and we consider the class C of smooth, radial and compactly supported electric potentials and magnetic fields denoted by V and B respectively. If (V, B) and (\tilde{V} , \tilde{B}) are two couples belonging to C, we then show that if the corresponding phase shifts $\delta$_l and \tilde{$\delta$}_l (i.e. the scattering data at fixed energy) coincide for all l $\in$ L, where L $\subset$ N^$\star$ satisfies the M{"u}ntz condition \sum_{l$\in$L} \frac{1}{l} = +$\mathrm{\infty }$, then V (x) = \tilde{V}(x) and B(x) = \tilde{B}(x) outside the obstacle B(0, r_0). The proof use the Complex Angular Momentum method and is close in spirit to the celebrated B{"o}rg-Marchenko uniqueness Theorem.