  ![Complex amplitude in $A$ and squared root of the amplitude in $D$, i.e. $|\mathcal{D}_n^m(r,\theta)|$. The parameters used in the simulation are: $\lambda f =0$, $R=0$, $d=0$, $\epsilon = 0$ (Lyot coronagraph). \[figresu0\]](f0a.eps "fig:"){width=".0\textwidth"}\ ![Complex amplitude in $A$ and squared root of the amplitude in $D$, i.e. $|\mathcal{D}_n^m(r,\theta)|$. The parameters used in the simulation are: $\lambda f =0$, $R=0$, $d=0$, $\epsilon = 0$ (Lyot coronagraph). \[figresu0\]](f0b.eps "fig:"){width=".0\textwidth"}\ ![Complex amplitude in $A$ and squared root of the amplitude in $D$, i.e. $|\mathcal{D}_n^m(r,\theta)|$. The parameters used in the simulation are: $\lambda f =0$, $R=0$, $d=0$, $\epsilon = 0$ (Lyot coronagraph). \[figresu0\]](f0c.eps "fig:"){width=".0\textwidth"}\  ![Complex amplitude in $A$ and squared root of the amplitude in $D$, i.e. $|\mathcal{D}_n^m(r,\theta)|$. The parameters used in the simulation are: $\lambda f =0$, $R=0$, $d=0$, $\epsilon = 0$ (Lyot coronagraph). \[figresu0\]](f0a.eps "fig:"){width=".0\textwidth"}\ ![Complex amplitude in $A$ and squared root of the amplitude in $D$, i.e. $|\mathcal{D}_n^m(r,\theta)|$. The parameters used in the simulation are: $\lambda f =0$, $R=0$, $d=0$, $\epsilon = 0$ (Lyot coronagraph). \[figresu0\]](f0b.eps "fig:"){width=".0\textwidth"}\ ![Complex amplitude in $A$ and squared root of the amplitude in $D$, i.e. $|\mathcal{D}_n^m(r,\theta)|$. The parameters used in the simulation are: $\lambda f =0$, $R=0$, $d=0$, $\epsilon = 0$ (Lyot coronagraph). \[figresu0\]](f0c.eps "fig:"){width=".0\textwidth"}\  ![