“…A list of such methods includes: -the method of surface integral equations [10], [11] -the method of auxiliary sources [12]; this method for twodimensional problems is easier than the method of surface integral equations, but it can be applied to the scatterers with smooth surfaces; -the method of integral equations for polarization currents [13], [14]; it is more universal than the previous two methods, since it allows analysis of inhomogeneous dielectric scatterers; -the finite-difference frequency-domain (FDFD) method [15], also allowing analysis of inhomogeneous scatterers; -the method of pattern equations [16], applicable only to homogeneous scatterers; its effectiveness is questionable, since [16] contains neither numerical results for comparisons with other methods; -the finite element method (FEM) [17] and its hybrid versions, for example [18], which are also universal; -the boundary element method [19]; and -a group of universal methods reducing the problem to systems of ordinary differential equations, including incomplete Galerkin method [20], unimoment method [21], method of coupled waves [22]- [24], used in [2], a modification of the coupled mode method combined with one-dimensional finite element method [25] and method of cross sections used in [26]. A hybrid projective method, relative to [25], was recently developed in [27] and [28] for analysis of one-dimensional periodic structures with wedge elements for application to matching layers and absorbing covers.…”