1. Introduction
Finite Differences (FD) [1] are among the most popular grid methods used in Computational Electrody-namics. They base on Maxwell equations written for discretized computational domain solved in time (Finite difference Time Domain (FDTD) method) or frequency (Finite Difference Frequency Domain (FDFD) method) domain. FD algorithms work under the assumption that fields between points change linearly, so to observe fields behaviors between grid points or apply a method that can improve FDTD or FDFD performance [2], [3] one often has to use interpolation.