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/* Copyright (C) 2005-2022 Massachusetts Institute of Technology
%
% This program 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, or (at your option)
% any later version.
%
% This program 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 this program; if not, write to the Free Software Foundation,
% Inc., 59 Temple Place - Suite 330, Boston, MA 02111-1307, USA.
*/
/* Check of Green's functions (analytical vs. numerical)
and near-to-far-field transformation. */
#include <stdio.h>
#include <stdlib.h>
#include "meep_internals.hpp"
using namespace meep;
using std::complex;
using std::polar;
double two(const vec &) { return 2.0; }
const int EHcomp[10] = {0, 1, 0, 1, 2, 3, 4, 3, 4, 5};
int check_cyl(double sr, double sz, double a) {
const double dpml = 1.0;
grid_volume gv = volcyl(sr + dpml, dpml + sz + dpml, a);
gv.center_origin();
component c0 = Ep;
master_printf("TESTING CYLINDRICAL AT RESOLUTION %g FOR %s SOURCE...\n", a, component_name(c0));
structure s(gv, two, pml(dpml));
double m = 0;
fields f(&s, m);
double w = 0.5;
continuous_src_time src(w);
vec x0 = veccyl(0.5 * sr, 0);
f.add_point_source(c0, src, x0);
f.solve_cw(sizeof(realnum) == sizeof(float) ? 1e-5 : 1e-6);
component c = Ep;
const int N = 20;
double dr = sr / N;
complex<double> F[N], F0[N], EH[6];
double diff = 0.0, dot0 = 0.0;
complex<double> phase = polar(1.0, (4 * w * f.dt) * pi);
for (int i = 0; i < N; ++i) {
double rr = dr * i;
vec x = veccyl(rr, 0.5 * sz);
F[i] = f.get_field(c, x) * phase;
greencyl(EH, x, w, 2.0, 1.0, x0, c0, 1.0, m, 1e-6);
F0[i] = EH[EHcomp[c]] * 2.0 * pi * x0.r(); // Ey = Ep for \phi = 0 (rz = xz) plane
double d = abs(F0[i] - F[i]);
double f0 = abs(F0[i]);
diff += d * d;
dot0 += f0 * f0;
}
double relerr = sqrt(diff) / sqrt(dot0);
master_printf(" GREEN: %s -> %s, resolution %g: relerr = %g\n", component_name(c0),
component_name(c), a, relerr);
if (relerr > 0.05 * 30 / a) {
for (int i = 0; i < N; ++i)
master_printf("%g, %g,%g, %g,%g\n", dr * i, real(F[i]), imag(F[i]), real(F0[i]), imag(F0[i]));
return 0;
}
volume_list vl = volume_list(
volume(veccyl(0, 0.5 * sz), veccyl(sr, 0.5 * sz)), Sz, 1.0,
new volume_list(
volume(veccyl(sr, 0.5 * sz), veccyl(sr, -0.5 * sz)), Sr, 1.0,
new volume_list(volume(veccyl(0, -0.5 * sz), veccyl(sr, -0.5 * sz)), Sz, -1.0)));
dft_near2far n2f = f.add_dft_near2far(&vl, w, w, 1);
f.update_dfts();
n2f.scale_dfts(sqrt(2 * pi) / f.dt); // cancel time-integration factor
complex<double> EH_[6];
diff = 0.0, dot0 = 0.0;
for (int i = 0; i < N; ++i) {
double rr = dr * i;
vec x = veccyl(rr, 10.0 / w);
n2f.farfield_lowlevel(EH_, x);
sum_to_all(EH_, EH, 6);
F[i] = EH[EHcomp[c]] * phase;
greencyl(EH, x, w, 2.0, 1.0, x0, c0, 1.0, m, 1e-6);
F0[i] = EH[EHcomp[c]] * 2.0 * pi * x0.r();
double d = abs(F0[i] - F[i]);
double f0 = abs(F0[i]);
diff += d * d;
dot0 += f0 * f0;
}
relerr = sqrt(diff) / sqrt(dot0);
master_printf(" NEAR2FAR: %s -> %s, resolution %g: relerr = %g\n", component_name(c0),
component_name(c), a, relerr);
if (relerr > 0.05 * 30 / a) {
for (int i = 0; i < N; ++i)
master_printf("%g, %g,%g, %g,%g\n", dr * i, real(F[i]), imag(F[i]), real(F0[i]), imag(F0[i]));
return 0;
}
return 1;
}
int check_2d_3d(ndim dim, const double xmax, double a, component c0, component c1 = NO_COMPONENT,
bool evenz = true) {
const double dpml = 1;
if (dim != D2 && dim != D3) meep::abort("2d or 3d required");
grid_volume gv = dim == D2 ? vol2d(xmax + 2 * dpml, xmax + 2 * dpml, a)
: vol3d(xmax + 2 * dpml, xmax + 2 * dpml, xmax + 2 * dpml, a);
gv.center_origin();
if (!gv.has_field(c0)) return 1;
if (c1 != NO_COMPONENT && !gv.has_field(c1)) return 1;
master_printf("TESTING %s AT RESOLUTION %g FOR %s SOURCE...\n", dim == D2 ? "2D" : "3D", a,
component_name(c0));
if (c1 != NO_COMPONENT) master_printf(" (and %s SOURCE)\n", component_name(c1));
// HACK: to speed up tests, we assume c0 and c1 have these symmetries
symmetry S = dim == D3 ? (evenz ? mirror(Z, gv) - mirror(X, gv) : mirror(X, gv) - mirror(Z, gv))
: (evenz ? -mirror(X, gv) : mirror(X, gv)); // 2d
structure s(gv, two, pml(dpml), S);
fields f(&s);
double w = 0.30;
continuous_src_time src(w);
f.add_point_source(c0, src, zero_vec(dim));
if (c1 != NO_COMPONENT) f.add_point_source(c1, src, zero_vec(dim), 0.7654321);
f.solve_cw(sizeof(realnum) == sizeof(float) ? 1e-5 : 1e-6);
FOR_E_AND_H(c) {
if (gv.has_field(c)) {
const int N = 20;
double dx = 0.75 * (xmax / 4) / N;
complex<double> F[N], F0[N], EH[6];
double diff = 0.0, dot0 = 0.0, dot = 0.0;
complex<double> phase = polar(1.0, (4 * w * f.dt) * pi);
vec x0 = zero_vec(dim);
for (int i = 0; i < N; ++i) {
double s = xmax / 4 + dx * i;
vec x = dim == D2 ? vec(s, 0.5 * s) : vec(s, 0.5 * s, 0.3 * s);
F[i] = f.get_field(c, x) * phase;
(dim == D2 ? green2d : green3d)(EH, x, w, 2.0, 1.0, x0, c0, 1.0);
F0[i] = EH[EHcomp[c]];
if (c1 != NO_COMPONENT) {
(dim == D2 ? green2d : green3d)(EH, x, w, 2.0, 1.0, x0, c1, 0.7654321);
F0[i] += EH[EHcomp[c]];
}
double d = abs(F0[i] - F[i]);
double f = abs(F[i]);
double f0 = abs(F0[i]);
diff += d * d;
dot += f * f;
dot0 += f0 * f0;
}
if (dot0 == 0) continue; /* zero field component */
double relerr = sqrt(diff) / sqrt(dot0);
master_printf(" GREEN: %s -> %s, resolution %g: relerr = %g\n", component_name(c0),
component_name(c), a, relerr);
if (relerr > 0.05 * 30 / a) {
for (int i = 0; i < N; ++i)
master_printf("%g, %g,%g, %g,%g\n", xmax / 4 + dx * i, real(F[i]), imag(F[i]),
real(F0[i]), imag(F0[i]));
return 0;
}
}
}
const double L = xmax / 4;
volume_list vl =
dim == D2
? volume_list(
volume(vec(-L, +L), vec(+L, +L)), Sy, 1.0,
new volume_list(
volume(vec(+L, +L), vec(+L, -L)), Sx, 1.0,
new volume_list(volume(vec(-L, -L), vec(+L, -L)), Sy, -1.0,
new volume_list(volume(vec(-L, -L), vec(-L, +L)), Sx, -1.0))))
: volume_list(volume(vec(+L, -L, -L), vec(+L, +L, +L)), Sx, +1.,
new volume_list(
volume(vec(-L, -L, -L), vec(-L, +L, +L)), Sx, -1.,
new volume_list(
volume(vec(-L, +L, -L), vec(+L, +L, +L)), Sy, +1.,
new volume_list(
volume(vec(-L, -L, -L), vec(+L, -L, +L)), Sy, -1.,
new volume_list(
volume(vec(-L, -L, +L), vec(+L, +L, +L)), Sz, +1.,
new volume_list(volume(vec(-L, -L, -L), vec(+L, +L, -L)),
Sz, -1.))))));
dft_near2far n2f = f.add_dft_near2far(&vl, w, w, 1);
f.update_dfts();
n2f.scale_dfts(sqrt(2 * pi) / f.dt); // cancel time-integration factor
FOR_E_AND_H(c) {
if (gv.has_field(c)) {
const int N = 20;
double dx = 0.75 * (xmax / 4) / N;
complex<double> F[N], F0[N], EH_[6], EH[6];
double diff = 0.0, dot = 0.0;
complex<double> phase = polar(1.0, (4 * w * f.dt) * pi);
vec x0 = zero_vec(dim);
for (int i = 0; i < N; ++i) {
double s = xmax + dx * i;
vec x = dim == D2 ? vec(s, 0.5 * s) : vec(s, 0.5 * s, 0.3 * s);
n2f.farfield_lowlevel(EH_, x);
sum_to_all(EH_, EH, 6);
F[i] = EH[EHcomp[c]] * phase;
(dim == D2 ? green2d : green3d)(EH, x, w, 2.0, 1.0, x0, c0, 1.0);
F0[i] = EH[EHcomp[c]];
if (c1 != NO_COMPONENT) {
(dim == D2 ? green2d : green3d)(EH, x, w, 2.0, 1.0, x0, c1, 0.7654321);
F0[i] += EH[EHcomp[c]];
}
double d = abs(F0[i] - F[i]);
double f0 = abs(F0[i]);
diff += d * d;
dot += f0 * f0;
}
if (dot == 0) continue; /* zero field component */
double relerr = sqrt(diff) / sqrt(dot);
master_printf(" NEAR2FAR: %s -> %s, resolution %g: relerr = %g\n", component_name(c0),
component_name(c), a, relerr);
if (relerr > 0.05 * 30 / a) {
for (int i = 0; i < N; ++i)
master_printf("%g, %g,%g, %g,%g\n", xmax + dx * i, real(F[i]), imag(F[i]), real(F0[i]),
imag(F0[i]));
return 0;
}
}
}
return 1;
}
int main(int argc, char **argv) {
initialize mpi(argc, argv);
const double a2d = argc > 1 ? atof(argv[1]) : 20, a3d = argc > 1 ? a2d : 10;
if ((sizeof(realnum) == sizeof(double)) && !check_cyl(5.0, 10.0, 20.0)) return 1;
// NOTE: see hack above -- we require sources to be odd in Z and even in X or vice-versa
if (!check_2d_3d(D3, 4, a3d, Ez, Hx, false)) return 1;
#if defined(HAVE_JN) || defined(HAVE_LIBGSL) // required for Hankel functions in 2d near2far
if (!check_2d_3d(D2, 8, a2d, Ez, Hx, false)) return 1;
if (!check_2d_3d(D2, 8, a2d, Ex, Hz, true)) return 1;
#endif
return 0;
}
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