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已同步 2025-08-07 23:14:03 +08:00
1283 行
51 KiB
Python
1283 行
51 KiB
Python
# Copyright (C) 2015-2024: The University of Edinburgh, United Kingdom
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# Authors: Craig Warren, Antonis Giannopoulos, and John Hartley
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#
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# This file is part of gprMax.
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#
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# gprMax is free software: you can redistribute it and/or modify
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# it under the terms of the GNU General Public License as published by
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# the Free Software Foundation, either version 3 of the License, or
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# (at your option) any later version.
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#
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# gprMax is distributed in the hope that it will be useful,
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# but WITHOUT ANY WARRANTY; without even the implied warranty of
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# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
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# GNU General Public License for more details.
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#
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# You should have received a copy of the GNU General Public License
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# along with gprMax. If not, see <http://www.gnu.org/licenses/>.
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from string import Template
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x_args = {
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"cuda": Template(
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"""
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__global__ void $FUNC(int xs,
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int xf,
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int ys,
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int yf,
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int zs,
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int zf,
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int NX_PHI1,
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int NY_PHI1,
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int NZ_PHI1,
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int NX_PHI2,
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int NY_PHI2,
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int NZ_PHI2,
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int NY_R,
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const unsigned int* __restrict__ ID,
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const $REAL* __restrict__ Ex,
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const $REAL* __restrict__ Ey,
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const $REAL* __restrict__ Ez,
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const $REAL* __restrict__ Hx,
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$REAL *Hy,
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$REAL *Hz,
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$REAL *PHI1,
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$REAL *PHI2,
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const $REAL* __restrict__ RA,
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const $REAL* __restrict__ RB,
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const $REAL* __restrict__ RE,
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const $REAL* __restrict__ RF,
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$REAL d)
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"""
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),
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"opencl": Template(
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"""
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int xs,
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int xf,
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int ys,
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int yf,
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int zs,
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int zf,
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int NX_PHI1,
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int NY_PHI1,
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int NZ_PHI1,
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int NX_PHI2,
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int NY_PHI2,
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int NZ_PHI2,
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int NY_R,
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__global const unsigned int* restrict ID,
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__global const $REAL* restrict Ex,
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__global const $REAL* restrict Ey,
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__global const $REAL* restrict Ez,
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__global const $REAL* restrict Hx,
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__global $REAL *Hy,
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__global $REAL *Hz,
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__global $REAL *PHI1,
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__global $REAL *PHI2,
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__global const $REAL* restrict RA,
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__global const $REAL* restrict RB,
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__global const $REAL* restrict RE,
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__global const $REAL* restrict RF,
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$REAL d
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"""
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),
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}
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y_args = {
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"cuda": Template(
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"""
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__global__ void $FUNC(int xs,
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int xf,
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int ys,
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int yf,
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int zs,
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int zf,
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int NX_PHI1,
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int NY_PHI1,
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int NZ_PHI1,
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int NX_PHI2,
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int NY_PHI2,
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int NZ_PHI2,
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int NY_R,
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const unsigned int* __restrict__ ID,
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const $REAL* __restrict__ Ex,
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const $REAL* __restrict__ Ey,
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const $REAL* __restrict__ Ez,
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$REAL *Hx,
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const $REAL* __restrict__ Hy,
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$REAL *Hz,
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$REAL *PHI1,
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$REAL *PHI2,
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const $REAL* __restrict__ RA,
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const $REAL* __restrict__ RB,
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const $REAL* __restrict__ RE,
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const $REAL* __restrict__ RF,
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$REAL d)
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"""
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),
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"opencl": Template(
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"""
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int xs,
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int xf,
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int ys,
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int yf,
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int zs,
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int zf,
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int NX_PHI1,
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int NY_PHI1,
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int NZ_PHI1,
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int NX_PHI2,
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int NY_PHI2,
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int NZ_PHI2,
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int NY_R,
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__global const unsigned int* restrict ID,
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__global const $REAL* restrict Ex,
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__global const $REAL* restrict Ey,
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__global const $REAL* restrict Ez,
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__global $REAL *Hx,
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__global const $REAL* restrict Hy,
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__global $REAL *Hz,
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__global $REAL *PHI1,
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__global $REAL *PHI2,
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__global const $REAL* restrict RA,
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__global const $REAL* restrict RB,
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__global const $REAL* restrict RE,
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__global const $REAL* restrict RF,
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$REAL d
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"""
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),
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}
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z_args = {
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"cuda": Template(
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"""
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__global__ void $FUNC(int xs,
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int xf,
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int ys,
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int yf,
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int zs,
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int zf,
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int NX_PHI1,
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int NY_PHI1,
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int NZ_PHI1,
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int NX_PHI2,
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int NY_PHI2,
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int NZ_PHI2,
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int NY_R,
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const unsigned int* __restrict__ ID,
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const $REAL* __restrict__ Ex,
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const $REAL* __restrict__ Ey,
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const $REAL* __restrict__ Ez,
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$REAL *Hx,
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$REAL *Hy,
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const $REAL* __restrict__ Hz,
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$REAL *PHI1,
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$REAL *PHI2,
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const $REAL* __restrict__ RA,
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const $REAL* __restrict__ RB,
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const $REAL* __restrict__ RE,
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const $REAL* __restrict__ RF,
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$REAL d)
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"""
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),
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"opencl": Template(
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"""
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int xs,
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int xf,
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int ys,
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int yf,
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int zs,
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int zf,
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int NX_PHI1,
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int NY_PHI1,
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int NZ_PHI1,
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int NX_PHI2,
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int NY_PHI2,
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int NZ_PHI2,
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int NY_R,
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__global const unsigned int* restrict ID,
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__global const $REAL* restrict Ex,
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__global const $REAL* restrict Ey,
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__global const $REAL* restrict Ez,
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__global $REAL *Hx,
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__global $REAL *Hy,
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__global const $REAL* restrict Hz,
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__global $REAL *PHI1,
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__global $REAL *PHI2,
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__global const $REAL* restrict RA,
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__global const $REAL* restrict RB,
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__global const $REAL* restrict RE,
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__global const $REAL* restrict RF,
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$REAL d
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"""
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),
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}
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order1_xminus = {
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"args_cuda": x_args["cuda"],
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"args_opencl": x_args["opencl"],
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"func": Template(
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"""
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// This function updates the Hy and Hz field components for the xminus slab.
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//
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// Args:
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// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
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// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
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// ID, E, H: Access to ID and field component arrays
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// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
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// d: Spatial discretisation, e.g. dx, dy or dz
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$CUDA_IDX
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// Convert the linear index to subscripts for PML PHI1 (4D) arrays
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int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
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int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
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int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
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int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
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// Convert the linear index to subscripts for PML PHI2 (4D) arrays
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int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
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int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
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int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
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int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
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$REAL IRA, IRA1, RB0, RC0, RE0, RF0, dEy, dEz;
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$REAL dx = d;
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int ii, jj, kk, materialHy, materialHz;
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int nx = xf - xs;
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int ny = yf - ys;
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int nz = zf - zs;
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if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
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// Subscripts for field arrays
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ii = xf - (i1 + 1);
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jj = j1 + ys;
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kk = k1 + zs;
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// PML coefficients
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IRA = 1 / RA[IDX2D_R(0,i1)];
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IRA1 = IRA - 1;
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RB0 = RB[IDX2D_R(0,i1)];
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RE0 = RE[IDX2D_R(0,i1)];
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RF0 = RF[IDX2D_R(0,i1)];
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RC0 = IRA * RB0 * RF0;
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// Hy
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materialHy = ID[IDX4D_ID(4,ii,jj,kk)];
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dEz = (Ez[IDX3D_FIELDS(ii+1,jj,kk)] - Ez[IDX3D_FIELDS(ii,jj,kk)]) / dx;
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Hy[IDX3D_FIELDS(ii,jj,kk)] = Hy[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHy,4)] *
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(IRA1 * dEz - IRA * PHI1[IDX4D_PHI1(0,i1,j1,k1)]);
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PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * dEz -
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RC0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)];
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}
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if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
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// Subscripts for field arrays
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ii = xf - (i2 + 1);
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jj = j2 + ys;
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kk = k2 + zs;
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// PML coefficients
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IRA = 1 / RA[IDX2D_R(0,i2)];
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IRA1 = IRA - 1;
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RB0 = RB[IDX2D_R(0,i2)];
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RE0 = RE[IDX2D_R(0,i2)];
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RF0 = RF[IDX2D_R(0,i2)];
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RC0 = IRA * RB0 * RF0;
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// Hz
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materialHz = ID[IDX4D_ID(5,ii,jj,kk)];
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dEy = (Ey[IDX3D_FIELDS(ii+1,jj,kk)] - Ey[IDX3D_FIELDS(ii,jj,kk)]) / dx;
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Hz[IDX3D_FIELDS(ii,jj,kk)] = Hz[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHz,4)] *
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(IRA1 * dEy - IRA * PHI2[IDX4D_PHI2(0,i2,j2,k2)]);
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PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * dEy -
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RC0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)];
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}
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"""
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),
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}
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order2_xminus = {
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"args_cuda": x_args["cuda"],
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"args_opencl": x_args["opencl"],
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"func": Template(
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"""
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// This function updates the Hy and Hz field components for the xminus slab.
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//
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// Args:
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// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
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// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
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// ID, E, H: Access to ID and field component arrays
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// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
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// d: Spatial discretisation, e.g. dx, dy or dz
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$CUDA_IDX
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// Convert the linear index to subscripts for PML PHI1 (4D) arrays
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int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
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int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
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int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
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int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
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// Convert the linear index to subscripts for PML PHI2 (4D) arrays
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int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
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int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
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int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
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int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
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$REAL IRA, IRA1, RB0, RC0, RE0, RF0, RB1, RC1, RE1, RF1, Psi1, Psi2, dEy, dEz;
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$REAL dx = d;
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int ii, jj, kk, materialHy, materialHz;
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int nx = xf - xs;
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int ny = yf - ys;
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int nz = zf - zs;
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if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
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// Subscripts for field arrays
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ii = xf - (i1 + 1);
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jj = j1 + ys;
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kk = k1 + zs;
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// PML coefficients
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IRA = 1 / (RA[IDX2D_R(0,i1)] + RA[IDX2D_R(1,i1)]);
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IRA1 = IRA - 1;
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RB0 = RB[IDX2D_R(0,i1)];
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RE0 = RE[IDX2D_R(0,i1)];
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RF0 = RF[IDX2D_R(0,i1)];
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RC0 = IRA * RF0;
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RB1 = RB[IDX2D_R(1,i1)];
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RE1 = RE[IDX2D_R(1,i1)];
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RF1 = RF[IDX2D_R(1,i1)];
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RC1 = IRA * RF1;
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// Hy
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Psi1 = RB0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RB1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)];
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materialHy = ID[IDX4D_ID(4,ii,jj,kk)];
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dEz = (Ez[IDX3D_FIELDS(ii+1,jj,kk)] - Ez[IDX3D_FIELDS(ii,jj,kk)]) / dx;
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Hy[IDX3D_FIELDS(ii,jj,kk)] = Hy[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHy,4)] *
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(IRA1 * dEz - IRA * Psi1);
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PHI1[IDX4D_PHI1(1,i1,j1,k1)] = RE1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)] + RC1 * (dEz - Psi1);
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PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * (dEz - Psi1);
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}
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if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
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// Subscripts for field arrays
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ii = xf - (i2 + 1);
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jj = j2 + ys;
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kk = k2 + zs;
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// PML coefficients
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IRA = 1 / (RA[IDX2D_R(0,i2)] + RA[IDX2D_R(1,i2)]);
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IRA1 = IRA - 1;
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RB0 = RB[IDX2D_R(0,i2)];
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RE0 = RE[IDX2D_R(0,i2)];
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RF0 = RF[IDX2D_R(0,i2)];
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RC0 = IRA * RF0;
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RB1 = RB[IDX2D_R(1,i2)];
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RE1 = RE[IDX2D_R(1,i2)];
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RF1 = RF[IDX2D_R(1,i2)];
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RC1 = IRA * RF1;
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// Hz
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Psi2 = RB0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RB1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)];
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materialHz = ID[IDX4D_ID(5,ii,jj,kk)];
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dEy = (Ey[IDX3D_FIELDS(ii+1,jj,kk)] - Ey[IDX3D_FIELDS(ii,jj,kk)]) / dx;
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Hz[IDX3D_FIELDS(ii,jj,kk)] = Hz[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHz,4)] *
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(IRA1 * dEy - IRA * Psi2);
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PHI2[IDX4D_PHI2(1,i2,j2,k2)] = RE1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)] + RC1 * (dEy - Psi2);
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PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * (dEy - Psi2);
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}
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"""
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),
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}
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order1_xplus = {
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"args_cuda": x_args["cuda"],
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"args_opencl": x_args["opencl"],
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"func": Template(
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"""
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// This function updates the Hy and Hz field components for the xplus slab.
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//
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// Args:
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// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
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// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
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// ID, E, H: Access to ID and field component arrays
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// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
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// d: Spatial discretisation, e.g. dx, dy or dz
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$CUDA_IDX
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// Convert the linear index to subscripts for PML PHI1 (4D) arrays
|
|
int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
|
|
int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
|
|
int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
|
|
int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
|
|
|
|
// Convert the linear index to subscripts for PML PHI2 (4D) arrays
|
|
int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
|
|
int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
|
|
int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
|
|
int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
|
|
|
|
$REAL IRA, IRA1, RB0, RC0, RE0, RF0, dEy, dEz;
|
|
$REAL dx = d;
|
|
int ii, jj, kk, materialHy, materialHz;
|
|
int nx = xf - xs;
|
|
int ny = yf - ys;
|
|
int nz = zf - zs;
|
|
|
|
if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i1 + xs;
|
|
jj = j1 + ys;
|
|
kk = k1 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / RA[IDX2D_R(0,i1)];
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,i1)];
|
|
RE0 = RE[IDX2D_R(0,i1)];
|
|
RF0 = RF[IDX2D_R(0,i1)];
|
|
RC0 = IRA * RB0 * RF0;
|
|
|
|
// Hy
|
|
materialHy = ID[IDX4D_ID(4,ii,jj,kk)];
|
|
dEz = (Ez[IDX3D_FIELDS(ii+1,jj,kk)] - Ez[IDX3D_FIELDS(ii,jj,kk)]) / dx;
|
|
Hy[IDX3D_FIELDS(ii,jj,kk)] = Hy[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHy,4)] *
|
|
(IRA1 * dEz - IRA * PHI1[IDX4D_PHI1(0,i1,j1,k1)]);
|
|
PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * dEz -
|
|
RC0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)];
|
|
}
|
|
|
|
if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i2 + xs;
|
|
jj = j2 + ys;
|
|
kk = k2 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / RA[IDX2D_R(0,i2)];
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,i2)];
|
|
RE0 = RE[IDX2D_R(0,i2)];
|
|
RF0 = RF[IDX2D_R(0,i2)];
|
|
RC0 = IRA * RB0 * RF0;
|
|
|
|
// Hz
|
|
materialHz = ID[IDX4D_ID(5,ii,jj,kk)];
|
|
dEy = (Ey[IDX3D_FIELDS(ii+1,jj,kk)] - Ey[IDX3D_FIELDS(ii,jj,kk)]) / dx;
|
|
Hz[IDX3D_FIELDS(ii,jj,kk)] = Hz[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHz,4)] *
|
|
(IRA1 * dEy - IRA * PHI2[IDX4D_PHI2(0,i2,j2,k2)]);
|
|
PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * dEy -
|
|
RC0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)];
|
|
}
|
|
"""
|
|
),
|
|
}
|
|
|
|
order2_xplus = {
|
|
"args_cuda": x_args["cuda"],
|
|
"args_opencl": x_args["opencl"],
|
|
"func": Template(
|
|
"""
|
|
// This function updates the Hy and Hz field components for the xplus slab.
|
|
//
|
|
// Args:
|
|
// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
|
|
// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
|
|
// ID, E, H: Access to ID and field component arrays
|
|
// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
|
|
// d: Spatial discretisation, e.g. dx, dy or dz
|
|
|
|
$CUDA_IDX
|
|
|
|
// Convert the linear index to subscripts for PML PHI1 (4D) arrays
|
|
int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
|
|
int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
|
|
int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
|
|
int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
|
|
|
|
// Convert the linear index to subscripts for PML PHI2 (4D) arrays
|
|
int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
|
|
int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
|
|
int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
|
|
int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
|
|
|
|
$REAL IRA, IRA1, RB0, RC0, RE0, RF0, RB1, RC1, RE1, RF1, Psi1, Psi2, dEy, dEz;
|
|
$REAL dx = d;
|
|
int ii, jj, kk, materialHy, materialHz;
|
|
int nx = xf - xs;
|
|
int ny = yf - ys;
|
|
int nz = zf - zs;
|
|
|
|
if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i1 + xs;
|
|
jj = j1 + ys;
|
|
kk = k1 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / (RA[IDX2D_R(0,i1)] + RA[IDX2D_R(1,i1)]);
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,i1)];
|
|
RE0 = RE[IDX2D_R(0,i1)];
|
|
RF0 = RF[IDX2D_R(0,i1)];
|
|
RC0 = IRA * RF0;
|
|
RB1 = RB[IDX2D_R(1,i1)];
|
|
RE1 = RE[IDX2D_R(1,i1)];
|
|
RF1 = RF[IDX2D_R(1,i1)];
|
|
RC1 = IRA * RF1;
|
|
|
|
// Hy
|
|
Psi1 = RB0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RB1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)];
|
|
materialHy = ID[IDX4D_ID(4,ii,jj,kk)];
|
|
dEz = (Ez[IDX3D_FIELDS(ii+1,jj,kk)] - Ez[IDX3D_FIELDS(ii,jj,kk)]) / dx;
|
|
Hy[IDX3D_FIELDS(ii,jj,kk)] = Hy[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHy,4)] *
|
|
(IRA1 * dEz - IRA * Psi1);
|
|
PHI1[IDX4D_PHI1(1,i1,j1,k1)] = RE1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)] + RC1 * (dEz - Psi1);
|
|
PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * (dEz - Psi1);
|
|
}
|
|
|
|
if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i2 + xs;
|
|
jj = j2 + ys;
|
|
kk = k2 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / (RA[IDX2D_R(0,i2)] + RA[IDX2D_R(1,i2)]);
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,i2)];
|
|
RE0 = RE[IDX2D_R(0,i2)];
|
|
RF0 = RF[IDX2D_R(0,i2)];
|
|
RC0 = IRA * RF0;
|
|
RB1 = RB[IDX2D_R(1,i2)];
|
|
RE1 = RE[IDX2D_R(1,i2)];
|
|
RF1 = RF[IDX2D_R(1,i2)];
|
|
RC1 = IRA * RF1;
|
|
|
|
// Hz
|
|
Psi2 = RB0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RB1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)];
|
|
materialHz = ID[IDX4D_ID(5,ii,jj,kk)];
|
|
dEy = (Ey[IDX3D_FIELDS(ii+1,jj,kk)] - Ey[IDX3D_FIELDS(ii,jj,kk)]) / dx;
|
|
Hz[IDX3D_FIELDS(ii,jj,kk)] = Hz[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHz,4)] *
|
|
(IRA1 * dEy - IRA * Psi2);
|
|
PHI2[IDX4D_PHI2(1,i2,j2,k2)] = RE1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)] + RC1 * (dEy - Psi2);
|
|
PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * (dEy - Psi2);
|
|
}
|
|
"""
|
|
),
|
|
}
|
|
|
|
order1_yminus = {
|
|
"args_cuda": y_args["cuda"],
|
|
"args_opencl": y_args["opencl"],
|
|
"func": Template(
|
|
"""
|
|
// This function updates the Hx and Hz field components for the yminus slab.
|
|
//
|
|
// Args:
|
|
// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
|
|
// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
|
|
// ID, E, H: Access to ID and field component arrays
|
|
// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
|
|
// d: Spatial discretisation, e.g. dx, dy or dz
|
|
|
|
$CUDA_IDX
|
|
|
|
// Convert the linear index to subscripts for PML PHI1 (4D) arrays
|
|
int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
|
|
int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
|
|
int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
|
|
int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
|
|
|
|
// Convert the linear index to subscripts for PML PHI2 (4D) arrays
|
|
int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
|
|
int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
|
|
int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
|
|
int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
|
|
|
|
$REAL IRA, IRA1, RB0, RC0, RE0, RF0, dEx, dEz;
|
|
$REAL dy = d;
|
|
int ii, jj, kk, materialHx, materialHz;
|
|
int nx = xf - xs;
|
|
int ny = yf - ys;
|
|
int nz = zf - zs;
|
|
|
|
if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i1 + xs;
|
|
jj = yf - (j1 + 1);
|
|
kk = k1 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / RA[IDX2D_R(0,j1)];
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,j1)];
|
|
RE0 = RE[IDX2D_R(0,j1)];
|
|
RF0 = RF[IDX2D_R(0,j1)];
|
|
RC0 = IRA * RB0 * RF0;
|
|
|
|
// Hx
|
|
materialHx = ID[IDX4D_ID(3,ii,jj,kk)];
|
|
dEz = (Ez[IDX3D_FIELDS(ii,jj+1,kk)] - Ez[IDX3D_FIELDS(ii,jj,kk)]) / dy;
|
|
Hx[IDX3D_FIELDS(ii,jj,kk)] = Hx[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHx,4)] *
|
|
(IRA1 * dEz - IRA * PHI1[IDX4D_PHI1(0,i1,j1,k1)]);
|
|
PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * dEz -
|
|
RC0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)];
|
|
}
|
|
|
|
if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i2 + xs;
|
|
jj = yf - (j2 + 1);
|
|
kk = k2 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / RA[IDX2D_R(0,j2)];
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,j2)];
|
|
RE0 = RE[IDX2D_R(0,j2)];
|
|
RF0 = RF[IDX2D_R(0,j2)];
|
|
RC0 = IRA * RB0 * RF0;
|
|
|
|
// Hz
|
|
materialHz = ID[IDX4D_ID(5,ii,jj,kk)];
|
|
dEx = (Ex[IDX3D_FIELDS(ii,jj+1,kk)] - Ex[IDX3D_FIELDS(ii,jj,kk)]) / dy;
|
|
Hz[IDX3D_FIELDS(ii,jj,kk)] = Hz[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHz,4)] *
|
|
(IRA1 * dEx - IRA * PHI2[IDX4D_PHI2(0,i2,j2,k2)]);
|
|
PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * dEx -
|
|
RC0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)];
|
|
}
|
|
"""
|
|
),
|
|
}
|
|
|
|
order2_yminus = {
|
|
"args_cuda": y_args["cuda"],
|
|
"args_opencl": y_args["opencl"],
|
|
"func": Template(
|
|
"""
|
|
// This function updates the Hx and Hz field components for the yminus slab.
|
|
//
|
|
// Args:
|
|
// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
|
|
// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
|
|
// ID, E, H: Access to ID and field component arrays
|
|
// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
|
|
// d: Spatial discretisation, e.g. dx, dy or dz
|
|
|
|
$CUDA_IDX
|
|
|
|
// Convert the linear index to subscripts for PML PHI1 (4D) arrays
|
|
int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
|
|
int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
|
|
int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
|
|
int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
|
|
|
|
// Convert the linear index to subscripts for PML PHI2 (4D) arrays
|
|
int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
|
|
int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
|
|
int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
|
|
int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
|
|
|
|
$REAL IRA, IRA1, RB0, RC0, RE0, RF0, RB1, RC1, RE1, RF1, Psi1, Psi2, dEx, dEz;
|
|
$REAL dy = d;
|
|
int ii, jj, kk, materialHx, materialHz;
|
|
int nx = xf - xs;
|
|
int ny = yf - ys;
|
|
int nz = zf - zs;
|
|
|
|
if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i1 + xs;
|
|
jj = yf - (j1 + 1);
|
|
kk = k1 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / (RA[IDX2D_R(0,j1)] + RA[IDX2D_R(1,j1)]);
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,j1)];
|
|
RE0 = RE[IDX2D_R(0,j1)];
|
|
RF0 = RF[IDX2D_R(0,j1)];
|
|
RC0 = IRA * RF0;
|
|
RB1 = RB[IDX2D_R(1,j1)];
|
|
RE1 = RE[IDX2D_R(1,j1)];
|
|
RF1 = RF[IDX2D_R(1,j1)];
|
|
RC1 = IRA * RF1;
|
|
|
|
// Hx
|
|
Psi1 = RB0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RB1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)];
|
|
materialHx = ID[IDX4D_ID(3,ii,jj,kk)];
|
|
dEz = (Ez[IDX3D_FIELDS(ii,jj+1,kk)] - Ez[IDX3D_FIELDS(ii,jj,kk)]) / dy;
|
|
Hx[IDX3D_FIELDS(ii,jj,kk)] = Hx[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHx,4)] *
|
|
(IRA1 * dEz - IRA * Psi1);
|
|
PHI1[IDX4D_PHI1(1,i1,j1,k1)] = RE1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)] + RC1 * (dEz - Psi1);
|
|
PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * (dEz - Psi1);
|
|
}
|
|
|
|
if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i2 + xs;
|
|
jj = yf - (j2 + 1);
|
|
kk = k2 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / (RA[IDX2D_R(0,j2)] + RA[IDX2D_R(1,j2)]);
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,j2)];
|
|
RE0 = RE[IDX2D_R(0,j2)];
|
|
RF0 = RF[IDX2D_R(0,j2)];
|
|
RC0 = IRA * RF0;
|
|
RB1 = RB[IDX2D_R(1,j2)];
|
|
RE1 = RE[IDX2D_R(1,j2)];
|
|
RF1 = RF[IDX2D_R(1,j2)];
|
|
RC1 = IRA * RF1;
|
|
|
|
// Hz
|
|
Psi2 = RB0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RB1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)];
|
|
materialHz = ID[IDX4D_ID(5,ii,jj,kk)];
|
|
dEx = (Ex[IDX3D_FIELDS(ii,jj+1,kk)] - Ex[IDX3D_FIELDS(ii,jj,kk)]) / dy;
|
|
Hz[IDX3D_FIELDS(ii,jj,kk)] = Hz[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHz,4)] *
|
|
(IRA1 * dEx - IRA * Psi2);
|
|
PHI2[IDX4D_PHI2(1,i2,j2,k2)] = RE1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)] + RC1 * (dEx - Psi2);
|
|
PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * (dEx - Psi2);
|
|
}
|
|
"""
|
|
),
|
|
}
|
|
|
|
order1_yplus = {
|
|
"args_cuda": y_args["cuda"],
|
|
"args_opencl": y_args["opencl"],
|
|
"func": Template(
|
|
"""
|
|
// This function updates the Hx and Hz field components for the yplus slab.
|
|
//
|
|
// Args:
|
|
// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
|
|
// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
|
|
// ID, E, H: Access to ID and field component arrays
|
|
// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
|
|
// d: Spatial discretisation, e.g. dx, dy or dz
|
|
|
|
$CUDA_IDX
|
|
|
|
// Convert the linear index to subscripts for PML PHI1 (4D) arrays
|
|
int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
|
|
int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
|
|
int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
|
|
int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
|
|
|
|
// Convert the linear index to subscripts for PML PHI2 (4D) arrays
|
|
int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
|
|
int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
|
|
int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
|
|
int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
|
|
|
|
$REAL IRA, IRA1, RB0, RC0, RE0, RF0, dEx, dEz;
|
|
$REAL dy = d;
|
|
int ii, jj, kk, materialHx, materialHz;
|
|
int nx = xf - xs;
|
|
int ny = yf - ys;
|
|
int nz = zf - zs;
|
|
|
|
if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i1 + xs;
|
|
jj = j1 + ys;
|
|
kk = k1 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / RA[IDX2D_R(0,j1)];
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,j1)];
|
|
RE0 = RE[IDX2D_R(0,j1)];
|
|
RF0 = RF[IDX2D_R(0,j1)];
|
|
RC0 = IRA * RB0 * RF0;
|
|
|
|
// Hx
|
|
materialHx = ID[IDX4D_ID(3,ii,jj,kk)];
|
|
dEz = (Ez[IDX3D_FIELDS(ii,jj+1,kk)] - Ez[IDX3D_FIELDS(ii,jj,kk)]) / dy;
|
|
Hx[IDX3D_FIELDS(ii,jj,kk)] = Hx[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHx,4)] *
|
|
(IRA1 * dEz - IRA * PHI1[IDX4D_PHI1(0,i1,j1,k1)]);
|
|
PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * dEz -
|
|
RC0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)];
|
|
}
|
|
|
|
if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i2 + xs;
|
|
jj = j2 + ys;
|
|
kk = k2 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / RA[IDX2D_R(0,j2)];
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,j2)];
|
|
RE0 = RE[IDX2D_R(0,j2)];
|
|
RF0 = RF[IDX2D_R(0,j2)];
|
|
RC0 = IRA * RB0 * RF0;
|
|
|
|
// Hz
|
|
materialHz = ID[IDX4D_ID(5,ii,jj,kk)];
|
|
dEx = (Ex[IDX3D_FIELDS(ii,jj+1,kk)] - Ex[IDX3D_FIELDS(ii,jj,kk)]) / dy;
|
|
Hz[IDX3D_FIELDS(ii,jj,kk)] = Hz[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHz,4)] *
|
|
(IRA1 * dEx - IRA * PHI2[IDX4D_PHI2(0,i2,j2,k2)]);
|
|
PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * dEx -
|
|
RC0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)];
|
|
}
|
|
"""
|
|
),
|
|
}
|
|
|
|
order2_yplus = {
|
|
"args_cuda": y_args["cuda"],
|
|
"args_opencl": y_args["opencl"],
|
|
"func": Template(
|
|
"""
|
|
// This function updates the Hx and Hz field components for the yplus slab.
|
|
//
|
|
// Args:
|
|
// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
|
|
// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
|
|
// ID, E, H: Access to ID and field component arrays
|
|
// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
|
|
// d: Spatial discretisation, e.g. dx, dy or dz
|
|
|
|
$CUDA_IDX
|
|
|
|
// Convert the linear index to subscripts for PML PHI1 (4D) arrays
|
|
int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
|
|
int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
|
|
int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
|
|
int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
|
|
|
|
// Convert the linear index to subscripts for PML PHI2 (4D) arrays
|
|
int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
|
|
int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
|
|
int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
|
|
int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
|
|
|
|
$REAL IRA, IRA1, RB0, RC0, RE0, RF0, RB1, RC1, RE1, RF1, Psi1, Psi2, dEx, dEz;
|
|
$REAL dy = d;
|
|
int ii, jj, kk, materialHx, materialHz;
|
|
int nx = xf - xs;
|
|
int ny = yf - ys;
|
|
int nz = zf - zs;
|
|
|
|
if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i1 + xs;
|
|
jj = j1 + ys;
|
|
kk = k1 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / (RA[IDX2D_R(0,j1)] + RA[IDX2D_R(1,j1)]);
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,j1)];
|
|
RE0 = RE[IDX2D_R(0,j1)];
|
|
RF0 = RF[IDX2D_R(0,j1)];
|
|
RC0 = IRA * RF0;
|
|
RB1 = RB[IDX2D_R(1,j1)];
|
|
RE1 = RE[IDX2D_R(1,j1)];
|
|
RF1 = RF[IDX2D_R(1,j1)];
|
|
RC1 = IRA * RF1;
|
|
|
|
// Hx
|
|
Psi1 = RB0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RB1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)];
|
|
materialHx = ID[IDX4D_ID(3,ii,jj,kk)];
|
|
dEz = (Ez[IDX3D_FIELDS(ii,jj+1,kk)] - Ez[IDX3D_FIELDS(ii,jj,kk)]) / dy;
|
|
Hx[IDX3D_FIELDS(ii,jj,kk)] = Hx[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHx,4)] *
|
|
(IRA1 * dEz - IRA * Psi1);
|
|
PHI1[IDX4D_PHI1(1,i1,j1,k1)] = RE1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)] + RC1 * (dEz - Psi1);
|
|
PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * (dEz - Psi1);
|
|
}
|
|
|
|
if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i2 + xs;
|
|
jj = j2 + ys;
|
|
kk = k2 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / (RA[IDX2D_R(0,j2)] + RA[IDX2D_R(1,j2)]);
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,j2)];
|
|
RE0 = RE[IDX2D_R(0,j2)];
|
|
RF0 = RF[IDX2D_R(0,j2)];
|
|
RC0 = IRA * RF0;
|
|
RB1 = RB[IDX2D_R(1,j2)];
|
|
RE1 = RE[IDX2D_R(1,j2)];
|
|
RF1 = RF[IDX2D_R(1,j2)];
|
|
RC1 = IRA * RF1;
|
|
|
|
// Hz
|
|
Psi2 = RB0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RB1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)];
|
|
materialHz = ID[IDX4D_ID(5,ii,jj,kk)];
|
|
dEx = (Ex[IDX3D_FIELDS(ii,jj+1,kk)] - Ex[IDX3D_FIELDS(ii,jj,kk)]) / dy;
|
|
Hz[IDX3D_FIELDS(ii,jj,kk)] = Hz[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHz,4)] *
|
|
(IRA1 * dEx - IRA * Psi2);
|
|
PHI2[IDX4D_PHI2(1,i2,j2,k2)] = RE1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)] + RC1 * (dEx - Psi2);
|
|
PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * (dEx - Psi2);
|
|
}
|
|
"""
|
|
),
|
|
}
|
|
|
|
order1_zminus = {
|
|
"args_cuda": z_args["cuda"],
|
|
"args_opencl": z_args["opencl"],
|
|
"func": Template(
|
|
"""
|
|
// This function updates the Hx and Hy field components for the zminus slab.
|
|
//
|
|
// Args:
|
|
// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
|
|
// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
|
|
// ID, E, H: Access to ID and field component arrays
|
|
// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
|
|
// d: Spatial discretisation, e.g. dx, dy or dz
|
|
|
|
$CUDA_IDX
|
|
|
|
// Convert the linear index to subscripts for PML PHI1 (4D) arrays
|
|
int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
|
|
int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
|
|
int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
|
|
int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
|
|
|
|
// Convert the linear index to subscripts for PML PHI2 (4D) arrays
|
|
int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
|
|
int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
|
|
int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
|
|
int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
|
|
|
|
$REAL IRA, IRA1, RB0, RC0, RE0, RF0, dEx, dEy;
|
|
$REAL dz = d;
|
|
int ii, jj, kk, materialHx, materialHy;
|
|
int nx = xf - xs;
|
|
int ny = yf - ys;
|
|
int nz = zf - zs;
|
|
|
|
if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i1 + xs;
|
|
jj = j1 + ys;
|
|
kk = zf - (k1 + 1);
|
|
|
|
// PML coefficients
|
|
IRA = 1 / RA[IDX2D_R(0,k1)];
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,k1)];
|
|
RE0 = RE[IDX2D_R(0,k1)];
|
|
RF0 = RF[IDX2D_R(0,k1)];
|
|
RC0 = IRA * RB0 * RF0;
|
|
|
|
// Hx
|
|
materialHx = ID[IDX4D_ID(3,ii,jj,kk)];
|
|
dEy = (Ey[IDX3D_FIELDS(ii,jj,kk+1)] - Ey[IDX3D_FIELDS(ii,jj,kk)]) / dz;
|
|
Hx[IDX3D_FIELDS(ii,jj,kk)] = Hx[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHx,4)] *
|
|
(IRA1 * dEy - IRA * PHI1[IDX4D_PHI1(0,i1,j1,k1)]);
|
|
PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * dEy -
|
|
RC0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)];
|
|
}
|
|
|
|
if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i2 + xs;
|
|
jj = j2 + ys;
|
|
kk = zf - (k2 + 1);
|
|
|
|
// PML coefficients
|
|
IRA = 1 / RA[IDX2D_R(0,k2)];
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,k2)];
|
|
RE0 = RE[IDX2D_R(0,k2)];
|
|
RF0 = RF[IDX2D_R(0,k2)];
|
|
RC0 = IRA * RB0 * RF0;
|
|
|
|
// Hy
|
|
materialHy = ID[IDX4D_ID(4,ii,jj,kk)];
|
|
dEx = (Ex[IDX3D_FIELDS(ii,jj,kk+1)] - Ex[IDX3D_FIELDS(ii,jj,kk)]) / dz;
|
|
Hy[IDX3D_FIELDS(ii,jj,kk)] = Hy[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHy,4)] *
|
|
(IRA1 * dEx - IRA * PHI2[IDX4D_PHI2(0,i2,j2,k2)]);
|
|
PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * dEx -
|
|
RC0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)];
|
|
}
|
|
"""
|
|
),
|
|
}
|
|
|
|
order2_zminus = {
|
|
"args_cuda": z_args["cuda"],
|
|
"args_opencl": z_args["opencl"],
|
|
"func": Template(
|
|
"""
|
|
// This function updates the Hx and Hy field components for the zminus slab.
|
|
//
|
|
// Args:
|
|
// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
|
|
// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
|
|
// ID, E, H: Access to ID and field component arrays
|
|
// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
|
|
// d: Spatial discretisation, e.g. dx, dy or dz
|
|
|
|
$CUDA_IDX
|
|
|
|
// Convert the linear index to subscripts for PML PHI1 (4D) arrays
|
|
int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
|
|
int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
|
|
int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
|
|
int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
|
|
|
|
// Convert the linear index to subscripts for PML PHI2 (4D) arrays
|
|
int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
|
|
int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
|
|
int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
|
|
int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
|
|
|
|
$REAL IRA, IRA1, RB0, RC0, RE0, RF0, RB1, RC1, RE1, RF1, Psi1, Psi2, dEx, dEy;
|
|
$REAL dz = d;
|
|
int ii, jj, kk, materialHx, materialHy;
|
|
int nx = xf - xs;
|
|
int ny = yf - ys;
|
|
int nz = zf - zs;
|
|
|
|
if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i1 + xs;
|
|
jj = j1 + ys;
|
|
kk = zf - (k1 + 1);
|
|
|
|
// PML coefficients
|
|
IRA = 1 / (RA[IDX2D_R(0,k1)] + RA[IDX2D_R(1,k1)]);
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,k1)];
|
|
RE0 = RE[IDX2D_R(0,k1)];
|
|
RF0 = RF[IDX2D_R(0,k1)];
|
|
RC0 = IRA * RF0;
|
|
RB1 = RB[IDX2D_R(1,k1)];
|
|
RE1 = RE[IDX2D_R(1,k1)];
|
|
RF1 = RF[IDX2D_R(1,k1)];
|
|
RC1 = IRA * RF1;
|
|
|
|
// Hx
|
|
Psi1 = RB0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RB1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)];
|
|
materialHx = ID[IDX4D_ID(3,ii,jj,kk)];
|
|
dEy = (Ey[IDX3D_FIELDS(ii,jj,kk+1)] - Ey[IDX3D_FIELDS(ii,jj,kk)]) / dz;
|
|
Hx[IDX3D_FIELDS(ii,jj,kk)] = Hx[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHx,4)] *
|
|
(IRA1 * dEy - IRA * Psi1);
|
|
PHI1[IDX4D_PHI1(1,i1,j1,k1)] = RE1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)] + RC1 * (dEy - Psi1);
|
|
PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * (dEy - Psi1);
|
|
}
|
|
|
|
if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i2 + xs;
|
|
jj = j2 + ys;
|
|
kk = zf - (k2 + 1);
|
|
|
|
// PML coefficients
|
|
IRA = 1 / (RA[IDX2D_R(0,k2)] + RA[IDX2D_R(1,k2)]);
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,k2)];
|
|
RE0 = RE[IDX2D_R(0,k2)];
|
|
RF0 = RF[IDX2D_R(0,k2)];
|
|
RC0 = IRA * RF0;
|
|
RB1 = RB[IDX2D_R(1,k2)];
|
|
RE1 = RE[IDX2D_R(1,k2)];
|
|
RF1 = RF[IDX2D_R(1,k2)];
|
|
RC1 = IRA * RF1;
|
|
|
|
// Hy
|
|
Psi2 = RB0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RB1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)];
|
|
materialHy = ID[IDX4D_ID(4,ii,jj,kk)];
|
|
dEx = (Ex[IDX3D_FIELDS(ii,jj,kk+1)] - Ex[IDX3D_FIELDS(ii,jj,kk)]) / dz;
|
|
Hy[IDX3D_FIELDS(ii,jj,kk)] = Hy[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHy,4)] *
|
|
(IRA1 * dEx - IRA * Psi2);
|
|
PHI2[IDX4D_PHI2(1,i2,j2,k2)] = RE1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)] + RC1 * (dEx - Psi2);
|
|
PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * (dEx - Psi2);
|
|
}
|
|
"""
|
|
),
|
|
}
|
|
|
|
order1_zplus = {
|
|
"args_cuda": z_args["cuda"],
|
|
"args_opencl": z_args["opencl"],
|
|
"func": Template(
|
|
"""
|
|
// This function updates the Hx and Hy field components for the zplus slab.
|
|
//
|
|
// Args:
|
|
// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
|
|
// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
|
|
// ID, E, H: Access to ID and field component arrays
|
|
// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
|
|
// d: Spatial discretisation, e.g. dx, dy or dz
|
|
|
|
$CUDA_IDX
|
|
|
|
// Convert the linear index to subscripts for PML PHI1 (4D) arrays
|
|
int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
|
|
int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
|
|
int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
|
|
int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
|
|
|
|
// Convert the linear index to subscripts for PML PHI2 (4D) arrays
|
|
int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
|
|
int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
|
|
int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
|
|
int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
|
|
|
|
$REAL IRA, IRA1, RB0, RC0, RE0, RF0, dEx, dEy;
|
|
$REAL dz = d;
|
|
int ii, jj, kk, materialHx, materialHy;
|
|
int nx = xf - xs;
|
|
int ny = yf - ys;
|
|
int nz = zf - zs;
|
|
|
|
if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i1 + xs;
|
|
jj = j1 + ys;
|
|
kk = k1 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / RA[IDX2D_R(0,k1)];
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,k1)];
|
|
RE0 = RE[IDX2D_R(0,k1)];
|
|
RF0 = RF[IDX2D_R(0,k1)];
|
|
RC0 = IRA * RB0 * RF0;
|
|
|
|
// Hx
|
|
materialHx = ID[IDX4D_ID(3,ii,jj,kk)];
|
|
dEy = (Ey[IDX3D_FIELDS(ii,jj,kk+1)] - Ey[IDX3D_FIELDS(ii,jj,kk)]) / dz;
|
|
Hx[IDX3D_FIELDS(ii,jj,kk)] = Hx[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHx,4)] *
|
|
(IRA1 * dEy - IRA * PHI1[IDX4D_PHI1(0,i1,j1,k1)]);
|
|
PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * dEy -
|
|
RC0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)];
|
|
}
|
|
|
|
if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i2 + xs;
|
|
jj = j2 + ys;
|
|
kk = k2 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / RA[IDX2D_R(0,k2)];
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,k2)];
|
|
RE0 = RE[IDX2D_R(0,k2)];
|
|
RF0 = RF[IDX2D_R(0,k2)];
|
|
RC0 = IRA * RB0 * RF0;
|
|
|
|
// Hy
|
|
materialHy = ID[IDX4D_ID(4,ii,jj,kk)];
|
|
dEx = (Ex[IDX3D_FIELDS(ii,jj,kk+1)] - Ex[IDX3D_FIELDS(ii,jj,kk)]) / dz;
|
|
Hy[IDX3D_FIELDS(ii,jj,kk)] = Hy[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHy,4)] *
|
|
(IRA1 * dEx - IRA * PHI2[IDX4D_PHI2(0,i2,j2,k2)]);
|
|
PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * dEx -
|
|
RC0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)];
|
|
}
|
|
"""
|
|
),
|
|
}
|
|
|
|
order2_zplus = {
|
|
"args_cuda": z_args["cuda"],
|
|
"args_opencl": z_args["opencl"],
|
|
"func": Template(
|
|
"""
|
|
// This function updates the Hx and Hy field components for the zplus slab.
|
|
//
|
|
// Args:
|
|
// xs, xf, ys, yf, zs, zf: Cell coordinates of PML slab
|
|
// NX_PHI, NY_PHI, NZ_PHI, NY_R: Dimensions of PHI1, PHI2, and R PML arrays
|
|
// ID, E, H: Access to ID and field component arrays
|
|
// Phi, RA, RB, RE, RF: Access to PML magnetic coefficient arrays
|
|
// d: Spatial discretisation, e.g. dx, dy or dz
|
|
|
|
$CUDA_IDX
|
|
|
|
// Convert the linear index to subscripts for PML PHI1 (4D) arrays
|
|
int p1 = i / (NX_PHI1 * NY_PHI1 * NZ_PHI1);
|
|
int i1 = (i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) / (NY_PHI1 * NZ_PHI1);
|
|
int j1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) / NZ_PHI1;
|
|
int k1 = ((i % (NX_PHI1 * NY_PHI1 * NZ_PHI1)) % (NY_PHI1 * NZ_PHI1)) % NZ_PHI1;
|
|
|
|
// Convert the linear index to subscripts for PML PHI2 (4D) arrays
|
|
int p2 = i / (NX_PHI2 * NY_PHI2 * NZ_PHI2);
|
|
int i2 = (i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) / (NY_PHI2 * NZ_PHI2);
|
|
int j2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) / NZ_PHI2;
|
|
int k2 = ((i % (NX_PHI2 * NY_PHI2 * NZ_PHI2)) % (NY_PHI2 * NZ_PHI2)) % NZ_PHI2;
|
|
|
|
$REAL IRA, IRA1, RB0, RC0, RE0, RF0, RB1, RC1, RE1, RF1, Psi1, Psi2, dEx, dEy;
|
|
$REAL dz = d;
|
|
int ii, jj, kk, materialHx, materialHy;
|
|
int nx = xf - xs;
|
|
int ny = yf - ys;
|
|
int nz = zf - zs;
|
|
|
|
if (p1 == 0 && i1 < nx && j1 < ny && k1 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i1 + xs;
|
|
jj = j1 + ys;
|
|
kk = k1 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / (RA[IDX2D_R(0,k1)] + RA[IDX2D_R(1,k1)]);
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,k1)];
|
|
RE0 = RE[IDX2D_R(0,k1)];
|
|
RF0 = RF[IDX2D_R(0,k1)];
|
|
RC0 = IRA * RF0;
|
|
RB1 = RB[IDX2D_R(1,k1)];
|
|
RE1 = RE[IDX2D_R(1,k1)];
|
|
RF1 = RF[IDX2D_R(1,k1)];
|
|
RC1 = IRA * RF1;
|
|
|
|
// Hx
|
|
Psi1 = RB0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RB1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)];
|
|
materialHx = ID[IDX4D_ID(3,ii,jj,kk)];
|
|
dEy = (Ey[IDX3D_FIELDS(ii,jj,kk+1)] - Ey[IDX3D_FIELDS(ii,jj,kk)]) / dz;
|
|
Hx[IDX3D_FIELDS(ii,jj,kk)] = Hx[IDX3D_FIELDS(ii,jj,kk)] + updatecoeffsH[IDX2D_MAT(materialHx,4)] *
|
|
(IRA1 * dEy - IRA * Psi1);
|
|
PHI1[IDX4D_PHI1(1,i1,j1,k1)] = RE1 * PHI1[IDX4D_PHI1(1,i1,j1,k1)] + RC1 * (dEy - Psi1);
|
|
PHI1[IDX4D_PHI1(0,i1,j1,k1)] = RE0 * PHI1[IDX4D_PHI1(0,i1,j1,k1)] + RC0 * (dEy - Psi1);
|
|
}
|
|
|
|
if (p2 == 0 && i2 < nx && j2 < ny && k2 < nz) {
|
|
// Subscripts for field arrays
|
|
ii = i2 + xs;
|
|
jj = j2 + ys;
|
|
kk = k2 + zs;
|
|
|
|
// PML coefficients
|
|
IRA = 1 / (RA[IDX2D_R(0,k2)] + RA[IDX2D_R(1,k2)]);
|
|
IRA1 = IRA - 1;
|
|
RB0 = RB[IDX2D_R(0,k2)];
|
|
RE0 = RE[IDX2D_R(0,k2)];
|
|
RF0 = RF[IDX2D_R(0,k2)];
|
|
RC0 = IRA * RF0;
|
|
RB1 = RB[IDX2D_R(1,k2)];
|
|
RE1 = RE[IDX2D_R(1,k2)];
|
|
RF1 = RF[IDX2D_R(1,k2)];
|
|
RC1 = IRA * RF1;
|
|
|
|
// Hy
|
|
Psi2 = RB0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RB1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)];
|
|
materialHy = ID[IDX4D_ID(4,ii,jj,kk)];
|
|
dEx = (Ex[IDX3D_FIELDS(ii,jj,kk+1)] - Ex[IDX3D_FIELDS(ii,jj,kk)]) / dz;
|
|
Hy[IDX3D_FIELDS(ii,jj,kk)] = Hy[IDX3D_FIELDS(ii,jj,kk)] - updatecoeffsH[IDX2D_MAT(materialHy,4)] *
|
|
(IRA1 * dEx - IRA * Psi2);
|
|
PHI2[IDX4D_PHI2(1,i2,j2,k2)] = RE1 * PHI2[IDX4D_PHI2(1,i2,j2,k2)] + RC1 * (dEx - Psi2);
|
|
PHI2[IDX4D_PHI2(0,i2,j2,k2)] = RE0 * PHI2[IDX4D_PHI2(0,i2,j2,k2)] + RC0 * (dEx - Psi2);
|
|
}
|
|
"""
|
|
),
|
|
}
|