PAR

Αιέν αριστεύειν καί υπείροχον έμμεναι άλλων, μηδέ γένος πατέρων αισχυνέμεν. (Homer, Iliad Z.208) Multilayered structures that include very thin conductive sheets have recently been techno-logically available and are receiving increased scientific interest within the Electromagnetic (EM) community. These conductive sheets can either be very thin compared to the operat-ing wavelength or even mono-atomically thick like in the case of graphene layers. In all the cases, its presence embedded within a multilayered structure represents a new EM challenge, since the standard computational EM solvers do not necessarily include these sheets in their definition of a stretched multilayered structure. One of the most suitable techniques for the EM modeling of multilayered structures is the Integral Equation technique solved with Method of Moments (IE-MoM) and more specifically the Mixed Potential Integral Equation (MPIE) formulation due to the lower order singularities in the kernels of the resulting integrals. The cornerstone of any IE formulation are th