%{ Copyright © 2020 Alexey A. Shcherbakov. All rights reserved. This file is part of GratingFMM. GratingFMM is free software: you can redistribute it and/or modify it under the terms of the GNU General Public License as published by the Free Software Foundation, either version 2 of the License, or (at your option) any later version. GratingFMM is distributed in the hope that it will be useful, but WITHOUT ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public License for more details. You should have received a copy of the GNU General Public License along with GratingFMM. If not, see . %} %% description: % calculate the power balance (check the energy conservation law) in case % of the collinear diffraction by 1D gratings % the returned value should be close to zero for pure dielectric structures % with no losses %% input: % no: number of Fourier harmonics % V_inc: incident field amplitude matrix of size (no, 2) % V_dif: diffracted field amplitude matrix of size (no, 2) % first index of V_inc, V_dif indicates diffraction harmonics % (0-th order index is ind_0 = ceil(no/2)) % second index of V_inc, V_dif, V_eff indicates whether the diffraction orders % are in the substrate (V(:,1)) or in the superstrate (V(:,2)) % kx0: incident plane wave wavevector x-projection (Bloch wavevector) % kg: wavelength-to-period ratio (grating vector) % eps1, eps2: substrate and superstrate permittivities % pol: polarization (either "TE" or "TM") %% output: % if the incident field has propagating harmonics the function returns the % normalized difference between the incident and diffractied field total % power, otherwise (if the incident field is purely evanescent) it returns % the total power carried by propagating diffraction orders %% implementation function [b] = fmm_balance(no, V_inc, V_dif, kx0, kg, eps1, eps2, pol) [kz1, kz2] = fmm_kxz(no, kx0, 0, kg, eps1, eps2); kz1 = transpose(kz1); kz2 = transpose(kz2); if (strcmp(pol,'TM')) kz1 = kz1/eps1; kz2 = kz2/eps2; end P_inc = sum( abs(V_inc(:,1).^2).*real(kz1) + abs(V_inc(:,2).^2).*real(kz2) ); P_dif = sum( abs(V_dif(:,1).^2).*real(kz1) + abs(V_dif(:,2).^2).*real(kz2) ); if (abs(P_inc) > 1e-15) b = abs(P_dif/P_inc-1); else b = 0.5*P_dif; end end % % END %