I. Introduction
A discrete geometric approach (DGA) of electromagnetic field problems is at the base of the fundamental works of T. Weiland with the finite integration technique (FIT) [1]–[3], E. Tonti with the Cell method (CM) [4]–[6] and A. Bossavit [8]–[11], [13]–[15], where a direct way of discretizing Maxwell equations is presented, alternative to the classical Galerkin methods in finite elements.