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937 lines
29 KiB
C++
937 lines
29 KiB
C++
#include "openmc/scattdata.h"
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#include <algorithm>
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#include <numeric>
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#include <cmath>
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#include "openmc/constants.h"
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#include "openmc/error.h"
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#include "openmc/math_functions.h"
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#include "openmc/random_lcg.h"
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namespace openmc {
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//==============================================================================
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// ScattData base-class methods
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//==============================================================================
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void
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ScattData::base_init(int order, const int_1dvec& in_gmin,
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const int_1dvec& in_gmax, const double_2dvec& in_energy,
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const double_2dvec& in_mult)
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{
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int groups = in_energy.size();
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gmin = in_gmin;
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gmax = in_gmax;
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energy.resize(groups);
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mult.resize(groups);
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dist.resize(groups);
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for (int gin = 0; gin < groups; gin++) {
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// Store the inputted data
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energy[gin] = in_energy[gin];
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mult[gin] = in_mult[gin];
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// Make sure the energy is normalized
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double norm = std::accumulate(energy[gin].begin(), energy[gin].end(), 0.);
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if (norm != 0.) {
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for (auto& n : energy[gin]) n /= norm;
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}
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// Initialize the distribution data
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dist[gin].resize(in_gmax[gin] - in_gmin[gin] + 1);
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for (auto& v : dist[gin]) {
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v.resize(order);
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}
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}
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}
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//==============================================================================
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void
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ScattData::base_combine(int max_order,
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const std::vector<ScattData*>& those_scatts, const double_1dvec& scalars,
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int_1dvec& in_gmin, int_1dvec& in_gmax, double_2dvec& sparse_mult,
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double_3dvec& sparse_scatter)
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{
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int groups = those_scatts[0] -> energy.size();
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// Now allocate and zero our storage spaces
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double_3dvec this_matrix = double_3dvec(groups, double_2dvec(groups,
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double_1dvec(max_order, 0.)));
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double_2dvec mult_numer(groups, double_1dvec(groups, 0.));
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double_2dvec mult_denom(groups, double_1dvec(groups, 0.));
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// Build the dense scattering and multiplicity matrices
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// Get the multiplicity_matrix
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// To combine from nuclidic data we need to use the final relationship
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// mult_{gg'} = sum_i(N_i*nuscatt_{i,g,g'}) /
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// sum_i(N_i*(nuscatt_{i,g,g'} / mult_{i,g,g'}))
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// Developed as follows:
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// mult_{gg'} = nuScatt{g,g'} / Scatt{g,g'}
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// mult_{gg'} = sum_i(N_i*nuscatt_{i,g,g'}) / sum(N_i*scatt_{i,g,g'})
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// mult_{gg'} = sum_i(N_i*nuscatt_{i,g,g'}) /
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// sum_i(N_i*(nuscatt_{i,g,g'} / mult_{i,g,g'}))
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// nuscatt_{i,g,g'} can be reconstructed from the energy and scattxs member
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// variables
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for (int i = 0; i < those_scatts.size(); i++) {
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ScattData* that = those_scatts[i];
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// Build the dense matrix for that object
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double_3dvec that_matrix = that->get_matrix(max_order);
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// Now add that to this for the scattering and multiplicity
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for (int gin = 0; gin < groups; gin++) {
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// Only spend time adding that's gmin to gmax data since the rest will
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// be zeros
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int i_gout = 0;
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for (int gout = that->gmin[gin]; gout <= that->gmax[gin]; gout++) {
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// Do the scattering matrix
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for (int l = 0; l < max_order; l++) {
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this_matrix[gin][gout][l] += scalars[i] * that_matrix[gin][gout][l];
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}
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// Incorporate that's contribution to the multiplicity matrix data
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double nuscatt = that->scattxs[gin] * that->energy[gin][i_gout];
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mult_numer[gin][gout] += scalars[i] * nuscatt;
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if (that->mult[gin][i_gout] > 0.) {
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mult_denom[gin][gout] += scalars[i] * nuscatt / that->mult[gin][i_gout];
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} else {
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mult_denom[gin][gout] += scalars[i];
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}
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i_gout++;
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}
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}
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}
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// Combine mult_numer and mult_denom into the combined multiplicity matrix
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double_2dvec this_mult(groups, double_1dvec(groups, 1.));
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for (int gin = 0; gin < groups; gin++) {
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for (int gout = 0; gout < groups; gout++) {
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if (mult_denom[gin][gout] > 0.) {
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this_mult[gin][gout] = mult_numer[gin][gout] / mult_denom[gin][gout];
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}
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}
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}
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mult_numer.clear();
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mult_denom.clear();
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// We have the data, now we need to convert to a jagged array and then use
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// the initialize function to store it on the object.
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for (int gin = 0; gin < groups; gin++) {
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// Find the minimum and maximum group boundaries
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int gmin_;
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for (gmin_ = 0; gmin_ < groups; gmin_++) {
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bool non_zero = false;
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for (int l = 0; l < this_matrix[gin][gmin_].size(); l++) {
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if (this_matrix[gin][gmin_][l] != 0.) {
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non_zero = true;
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break;
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}
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}
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if (non_zero) break;
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}
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int gmax_;
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for (gmax_ = groups - 1; gmax_ >= 0; gmax_--) {
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bool non_zero = false;
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for (int l = 0; l < this_matrix[gin][gmax_].size(); l++) {
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if (this_matrix[gin][gmax_][l] != 0.) {
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non_zero = true;
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break;
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}
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}
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if (non_zero) break;
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}
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// treat the case of all values being 0
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if (gmin_ > gmax_) {
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gmin_ = gin;
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gmax_ = gin;
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}
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// Store the group bounds
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in_gmin[gin] = gmin_;
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in_gmax[gin] = gmax_;
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// Store the data in the compressed format
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sparse_scatter[gin].resize(gmax_ - gmin_ + 1);
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sparse_mult[gin].resize(gmax_ - gmin_ + 1);
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int i_gout = 0;
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for (int gout = gmin_; gout <= gmax_; gout++) {
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sparse_scatter[gin][i_gout] = this_matrix[gin][gout];
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sparse_mult[gin][i_gout] = this_mult[gin][gout];
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i_gout++;
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}
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}
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}
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//==============================================================================
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void
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ScattData::sample_energy(int gin, int& gout, int& i_gout)
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{
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// Sample the outgoing group
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double xi = prn();
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i_gout = 0;
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gout = gmin[gin];
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double prob = energy[gin][i_gout];
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while((prob < xi) && (gout < gmax[gin])) {
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gout++;
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i_gout++;
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prob += energy[gin][i_gout];
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}
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}
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//==============================================================================
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double
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ScattData::get_xs(int xstype, int gin, const int* gout, const double* mu)
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{
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// Set the outgoing group offset index as needed
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int i_gout = 0;
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if (gout != nullptr) {
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// short circuit the function if gout is from a zero portion of the
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// scattering matrix
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if ((*gout < gmin[gin]) || (*gout > gmax[gin])) { // > gmax?
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return 0.;
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}
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i_gout = *gout - gmin[gin];
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}
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double val = scattxs[gin];
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switch(xstype) {
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case MG_GET_XS_SCATTER:
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if (gout != nullptr) val *= energy[gin][i_gout];
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break;
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case MG_GET_XS_SCATTER_MULT:
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if (gout != nullptr) {
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val *= energy[gin][i_gout] / mult[gin][i_gout];
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} else {
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val /= std::inner_product(mult[gin].begin(), mult[gin].end(),
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energy[gin].begin(), 0.0);
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}
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break;
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case MG_GET_XS_SCATTER_FMU_MULT:
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if ((gout != nullptr) && (mu != nullptr)) {
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val *= energy[gin][i_gout] * calc_f(gin, *gout, *mu);
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} else {
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// This is not an expected path (asking for f_mu without asking for a
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// group or mu is not useful
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fatal_error("Invalid call to get_xs");
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}
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break;
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case MG_GET_XS_SCATTER_FMU:
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if ((gout != nullptr) && (mu != nullptr)) {
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val *= energy[gin][i_gout] * calc_f(gin, *gout, *mu) / mult[gin][i_gout];
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} else {
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// This is not an expected path (asking for f_mu without asking for a
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// group or mu is not useful
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fatal_error("Invalid call to get_xs");
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}
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break;
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}
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return val;
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}
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//==============================================================================
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// ScattDataLegendre methods
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//==============================================================================
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void
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ScattDataLegendre::init(const int_1dvec& in_gmin, const int_1dvec& in_gmax,
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const double_2dvec& in_mult, const double_3dvec& coeffs)
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{
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int groups = coeffs.size();
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int order = coeffs[0][0].size();
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// make a copy of coeffs that we can use to both extract data and normalize
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double_3dvec matrix = coeffs;
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// Get the scattering cross section value by summing the un-normalized P0
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// coefficient in the variable matrix over all outgoing groups.
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scattxs.resize(groups);
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for (int gin = 0; gin < groups; gin++) {
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int num_groups = in_gmax[gin] - in_gmin[gin] + 1;
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scattxs[gin] = 0.;
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for (int i_gout = 0; i_gout < num_groups; i_gout++) {
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scattxs[gin] += matrix[gin][i_gout][0];
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}
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}
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// Build the energy transfer matrix from data in the variable matrix while
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// also normalizing the variable matrix itself
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// (forcing the CDF of f(mu=1) == 1)
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double_2dvec in_energy;
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in_energy.resize(groups);
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for (int gin = 0; gin < groups; gin++) {
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int num_groups = in_gmax[gin] - in_gmin[gin] + 1;
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in_energy[gin].resize(num_groups);
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for (int i_gout = 0; i_gout < num_groups; i_gout++) {
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double norm = matrix[gin][i_gout][0];
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in_energy[gin][i_gout] = norm;
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if (norm != 0.) {
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for (auto& n : matrix[gin][i_gout]) n /= norm;
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}
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}
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}
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// Initialize the base class attributes
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ScattData::base_init(order, in_gmin, in_gmax, in_energy, in_mult);
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// Set the distribution (sdata.dist) values and initialize max_val
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max_val.resize(groups);
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for (int gin = 0; gin < groups; gin++) {
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int num_groups = gmax[gin] - gmin[gin] + 1;
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for (int i_gout = 0; i_gout < num_groups; i_gout++) {
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dist[gin][i_gout] = matrix[gin][i_gout];
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}
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max_val[gin].resize(num_groups);
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for (auto& n : max_val[gin]) n = 0.;
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}
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// Now update the maximum value
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update_max_val();
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}
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//==============================================================================
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void
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ScattDataLegendre::update_max_val()
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{
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int groups = max_val.size();
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// Step through the polynomial with fixed number of points to identify the
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// maximal value
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int Nmu = 1001;
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double dmu = 2. / (Nmu - 1);
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for (int gin = 0; gin < groups; gin++) {
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int num_groups = gmax[gin] - gmin[gin] + 1;
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for (int i_gout = 0; i_gout < num_groups; i_gout++) {
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for (int imu = 0; imu < Nmu; imu++) {
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double mu;
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if (imu == 0) {
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mu = -1.;
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} else if (imu == (Nmu - 1)) {
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mu = 1.;
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} else {
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mu = -1. + (imu - 1) * dmu;
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}
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// Calculate probability
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double f = evaluate_legendre_c(dist[gin][i_gout].size() - 1,
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dist[gin][i_gout].data(), mu);
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// if this is a new maximum, store it
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if (f > max_val[gin][i_gout]) max_val[gin][i_gout] = f;
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} // end imu loop
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// Since we may not have caught the true max, add 10% margin
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max_val[gin][i_gout] *= 1.1;
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}
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}
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}
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//==============================================================================
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double
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ScattDataLegendre::calc_f(int gin, int gout, double mu)
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{
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double f;
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if ((gout < gmin[gin]) || (gout > gmax[gin])) {
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f = 0.;
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} else {
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int i_gout = gout - gmin[gin];
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f = evaluate_legendre_c(dist[gin][i_gout].size() - 1,
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dist[gin][i_gout].data(), mu);
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}
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return f;
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}
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//==============================================================================
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void
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ScattDataLegendre::sample(int gin, int& gout, double& mu, double& wgt)
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{
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// Sample the outgoing energy using the base-class method
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int i_gout;
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sample_energy(gin, gout, i_gout);
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// Now we can sample mu using the scattering kernel using rejection
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// sampling from a rectangular bounding box
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double M = max_val[gin][i_gout];
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int samples = 0;
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while(true) {
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mu = 2. * prn() - 1.;
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double f = calc_f(gin, gout, mu);
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if (f > 0.) {
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double u = prn() * M;
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if (u <= f) break;
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}
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samples++;
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if (samples > MAX_SAMPLE) {
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fatal_error("Maximum number of Legendre expansion samples reached");
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}
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};
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// Update the weight to reflect neutron multiplicity
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wgt *= mult[gin][i_gout];
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}
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//==============================================================================
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void
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ScattDataLegendre::combine(const std::vector<ScattData*>& those_scatts,
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const double_1dvec& scalars)
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{
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// Find the max order in the data set and make sure we can combine the sets
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int max_order = 0;
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for (int i = 0; i < those_scatts.size(); i++) {
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// Lets also make sure these items are combineable
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ScattDataLegendre* that = dynamic_cast<ScattDataLegendre*>(those_scatts[i]);
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if (!that) {
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fatal_error("Cannot combine the ScattData objects!");
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}
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int that_order = that->get_order();
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if (that_order > max_order) max_order = that_order;
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}
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max_order++; // Add one since this is a Legendre
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int groups = those_scatts[0] -> energy.size();
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int_1dvec in_gmin(groups);
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int_1dvec in_gmax(groups);
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double_3dvec sparse_scatter(groups);
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double_2dvec sparse_mult(groups);
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// The rest of the steps do not depend on the type of angular representation
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// so we use a base class method to sum up xs and create new energy and mult
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// matrices
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ScattData::base_combine(max_order, those_scatts, scalars, in_gmin, in_gmax,
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sparse_mult, sparse_scatter);
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// Got everything we need, store it.
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init(in_gmin, in_gmax, sparse_mult, sparse_scatter);
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}
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//==============================================================================
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double_3dvec
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ScattDataLegendre::get_matrix(int max_order)
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{
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// Get the sizes and initialize the data to 0
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int groups = energy.size();
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int order_dim = max_order + 1;
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double_3dvec matrix = double_3dvec(groups, double_2dvec(groups,
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double_1dvec(order_dim, 0.)));
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for (int gin = 0; gin < groups; gin++) {
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for (int i_gout = 0; i_gout < energy[gin].size(); i_gout++) {
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int gout = i_gout + gmin[gin];
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for (int l = 0; l < order_dim; l++) {
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matrix[gin][gout][l] = scattxs[gin] * energy[gin][i_gout] *
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dist[gin][i_gout][l];
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}
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}
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}
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return matrix;
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}
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//==============================================================================
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// ScattDataHistogram methods
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//==============================================================================
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void
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ScattDataHistogram::init(const int_1dvec& in_gmin, const int_1dvec& in_gmax,
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const double_2dvec& in_mult, const double_3dvec& coeffs)
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{
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int groups = coeffs.size();
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int order = coeffs[0][0].size();
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// make a copy of coeffs that we can use to both extract data and normalize
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double_3dvec matrix = coeffs;
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// Get the scattering cross section value by summing the distribution
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// over all the histogram bins in angle and outgoing energy groups
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scattxs.resize(groups);
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for (int gin = 0; gin < groups; gin++) {
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scattxs[gin] = 0.;
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for (int i_gout = 0; i_gout < matrix[gin].size(); i_gout++) {
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scattxs[gin] += std::accumulate(matrix[gin][i_gout].begin(),
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matrix[gin][i_gout].end(), 0.);
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}
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}
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// Build the energy transfer matrix from data in the variable matrix
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double_2dvec in_energy;
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in_energy.resize(groups);
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for (int gin = 0; gin < groups; gin++) {
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int num_groups = in_gmax[gin] - in_gmin[gin] + 1;
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in_energy[gin].resize(num_groups);
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for (int i_gout = 0; i_gout < num_groups; i_gout++) {
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double norm = std::accumulate(matrix[gin][i_gout].begin(),
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matrix[gin][i_gout].end(), 0.);
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in_energy[gin][i_gout] = norm;
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if (norm != 0.) {
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for (auto& n : matrix[gin][i_gout]) n /= norm;
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}
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}
|
|
}
|
|
|
|
// Initialize the base class attributes
|
|
ScattData::base_init(order, in_gmin, in_gmax, in_energy, in_mult);
|
|
|
|
// Build the angular distribution mu values
|
|
mu = double_1dvec(order);
|
|
dmu = 2. / order;
|
|
mu[0] = -1.;
|
|
for (int imu = 1; imu < order; imu++) {
|
|
mu[imu] = -1. + imu * dmu;
|
|
}
|
|
|
|
// Calculate f(mu) and integrate it so we can avoid rejection sampling
|
|
fmu.resize(groups);
|
|
for (int gin = 0; gin < groups; gin++) {
|
|
int num_groups = gmax[gin] - gmin[gin] + 1;
|
|
fmu[gin].resize(num_groups);
|
|
for (int i_gout = 0; i_gout < num_groups; i_gout++) {
|
|
fmu[gin][i_gout].resize(order);
|
|
// The variable matrix contains f(mu); so directly assign it
|
|
fmu[gin][i_gout] = matrix[gin][i_gout];
|
|
|
|
// Integrate the histogram
|
|
dist[gin][i_gout][0] = dmu * matrix[gin][i_gout][0];
|
|
for (int imu = 1; imu < order; imu++) {
|
|
dist[gin][i_gout][imu] = dmu * matrix[gin][i_gout][imu] +
|
|
dist[gin][i_gout][imu - 1];
|
|
}
|
|
|
|
// Now re-normalize for integral to unity
|
|
double norm = dist[gin][i_gout][order - 1];
|
|
if (norm > 0.) {
|
|
for (int imu = 0; imu < order; imu++) {
|
|
fmu[gin][i_gout][imu] /= norm;
|
|
dist[gin][i_gout][imu] /= norm;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
|
|
//==============================================================================
|
|
|
|
double
|
|
ScattDataHistogram::calc_f(int gin, int gout, double mu)
|
|
{
|
|
double f;
|
|
if ((gout < gmin[gin]) || (gout > gmax[gin])) {
|
|
f = 0.;
|
|
} else {
|
|
// Find mu bin
|
|
int i_gout = gout - gmin[gin];
|
|
int imu;
|
|
if (mu == 1.) {
|
|
// use size -2 to have the index one before the end
|
|
imu = this->mu.size() - 2;
|
|
} else {
|
|
imu = std::floor((mu + 1.) / dmu + 1.) - 1;
|
|
}
|
|
|
|
f = fmu[gin][i_gout][imu];
|
|
}
|
|
return f;
|
|
}
|
|
|
|
//==============================================================================
|
|
|
|
void
|
|
ScattDataHistogram::sample(int gin, int& gout, double& mu, double& wgt)
|
|
{
|
|
// Sample the outgoing energy using the base-class method
|
|
int i_gout;
|
|
sample_energy(gin, gout, i_gout);
|
|
|
|
// Determine the outgoing cosine bin
|
|
double xi = prn();
|
|
|
|
int imu;
|
|
if (xi < dist[gin][i_gout][0]) {
|
|
imu = 0;
|
|
} else {
|
|
// TODO lower_bound? + 1?
|
|
imu = std::upper_bound(dist[gin][i_gout].begin(),
|
|
dist[gin][i_gout].end(), xi) -
|
|
dist[gin][i_gout].begin();
|
|
}
|
|
|
|
// Randomly select mu within the imu bin
|
|
mu = prn() * dmu + this->mu[imu];
|
|
|
|
if (mu < -1.) {
|
|
mu = -1.;
|
|
} else if (mu > 1.) {
|
|
mu = 1.;
|
|
}
|
|
|
|
// Update the weight to reflect neutron multiplicity
|
|
wgt *= mult[gin][i_gout];
|
|
}
|
|
|
|
//==============================================================================
|
|
|
|
double_3dvec
|
|
ScattDataHistogram::get_matrix(int max_order)
|
|
{
|
|
// Get the sizes and initialize the data to 0
|
|
int groups = energy.size();
|
|
// We ignore the requested order for Histogram and Tabular representations
|
|
int order_dim = get_order();
|
|
double_3dvec matrix = double_3dvec(groups, double_2dvec(groups,
|
|
double_1dvec(order_dim, 0.)));
|
|
|
|
for (int gin = 0; gin < groups; gin++) {
|
|
for (int i_gout = 0; i_gout < energy[gin].size(); i_gout++) {
|
|
int gout = i_gout + gmin[gin];
|
|
for (int l = 0; l < order_dim; l++) {
|
|
matrix[gin][gout][l] = scattxs[gin] * energy[gin][i_gout] *
|
|
fmu[gin][i_gout][l];
|
|
}
|
|
}
|
|
}
|
|
return matrix;
|
|
}
|
|
|
|
//==============================================================================
|
|
|
|
void
|
|
ScattDataHistogram::combine(const std::vector<ScattData*>& those_scatts,
|
|
const double_1dvec& scalars)
|
|
{
|
|
// Find the max order in the data set and make sure we can combine the sets
|
|
int max_order = those_scatts[0]->get_order();
|
|
for (int i = 0; i < those_scatts.size(); i++) {
|
|
// Lets also make sure these items are combineable
|
|
ScattDataHistogram* that = dynamic_cast<ScattDataHistogram*>(those_scatts[i]);
|
|
if (!that) {
|
|
fatal_error("Cannot combine the ScattData objects!");
|
|
}
|
|
if (max_order != that->get_order()) {
|
|
fatal_error("Cannot combine the ScattData objects!");
|
|
}
|
|
}
|
|
|
|
int groups = those_scatts[0] -> energy.size();
|
|
|
|
int_1dvec in_gmin(groups);
|
|
int_1dvec in_gmax(groups);
|
|
double_3dvec sparse_scatter(groups);
|
|
double_2dvec sparse_mult(groups);
|
|
|
|
// The rest of the steps do not depend on the type of angular representation
|
|
// so we use a base class method to sum up xs and create new energy and mult
|
|
// matrices
|
|
ScattData::base_combine(max_order, those_scatts, scalars, in_gmin, in_gmax,
|
|
sparse_mult, sparse_scatter);
|
|
|
|
// Got everything we need, store it.
|
|
init(in_gmin, in_gmax, sparse_mult, sparse_scatter);
|
|
}
|
|
|
|
//==============================================================================
|
|
// ScattDataTabular methods
|
|
//==============================================================================
|
|
|
|
void
|
|
ScattDataTabular::init(const int_1dvec& in_gmin, const int_1dvec& in_gmax,
|
|
const double_2dvec& in_mult, const double_3dvec& coeffs)
|
|
{
|
|
int groups = coeffs.size();
|
|
int order = coeffs[0][0].size();
|
|
|
|
// make a copy of coeffs that we can use to both extract data and normalize
|
|
double_3dvec matrix = coeffs;
|
|
|
|
// Build the angular distribution mu values
|
|
mu = double_1dvec(order);
|
|
dmu = 2. / (order - 1);
|
|
mu[0] = -1.;
|
|
for (int imu = 1; imu < order - 1; imu++) {
|
|
mu[imu] = -1. + imu * dmu;
|
|
}
|
|
mu[order - 1] = 1.;
|
|
|
|
// Get the scattering cross section value by integrating the distribution
|
|
// over all mu points and then combining over all outgoing groups
|
|
scattxs.resize(groups);
|
|
for (int gin = 0; gin < groups; gin++) {
|
|
scattxs[gin] = 0.;
|
|
for (int i_gout = 0; i_gout < matrix[gin].size(); i_gout++) {
|
|
for (int imu = 1; imu < order; imu++) {
|
|
scattxs[gin] += 0.5 * dmu * (matrix[gin][i_gout][imu - 1] +
|
|
matrix[gin][i_gout][imu]);
|
|
}
|
|
}
|
|
}
|
|
|
|
// Build the energy transfer matrix from data in the variable matrix
|
|
double_2dvec in_energy(groups);
|
|
for (int gin = 0; gin < groups; gin++) {
|
|
int num_groups = in_gmax[gin] - in_gmin[gin] + 1;
|
|
in_energy[gin].resize(num_groups);
|
|
for (int i_gout = 0; i_gout < num_groups; i_gout++) {
|
|
double norm = 0.;
|
|
for (int imu = 1; imu < order; imu++) {
|
|
norm += 0.5 * dmu * (matrix[gin][i_gout][imu - 1] +
|
|
matrix[gin][i_gout][imu]);
|
|
}
|
|
in_energy[gin][i_gout] = norm;
|
|
}
|
|
}
|
|
|
|
// Initialize the base class attributes
|
|
ScattData::base_init(order, in_gmin, in_gmax, in_energy, in_mult);
|
|
|
|
// Calculate f(mu) and integrate it so we can avoid rejection sampling
|
|
fmu.resize(groups);
|
|
for (int gin = 0; gin < groups; gin++) {
|
|
int num_groups = gmax[gin] - gmin[gin] + 1;
|
|
fmu[gin].resize(num_groups);
|
|
for (int i_gout = 0; i_gout < num_groups; i_gout++) {
|
|
fmu[gin][i_gout].resize(order);
|
|
// The variable matrix contains f(mu); so directly assign it
|
|
fmu[gin][i_gout] = matrix[gin][i_gout];
|
|
|
|
// Ensure positivity
|
|
for (auto& val : fmu[gin][i_gout]) {
|
|
if (val < 0.) val = 0.;
|
|
}
|
|
|
|
// Now re-normalize for numerical integration issues and to take care of
|
|
// the above negative fix-up. Also accrue the CDF
|
|
double norm = 0.;
|
|
for (int imu = 1; imu < order; imu++) {
|
|
norm += 0.5 * dmu * (fmu[gin][i_gout][imu - 1] +
|
|
fmu[gin][i_gout][imu]);
|
|
// incorporate to the CDF
|
|
dist[gin][i_gout][imu] = norm;
|
|
}
|
|
|
|
// now do the normalization
|
|
if (norm > 0.) {
|
|
for (int imu = 0; imu < order; imu++) {
|
|
fmu[gin][i_gout][imu] /= norm;
|
|
dist[gin][i_gout][imu] /= norm;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
|
|
//==============================================================================
|
|
|
|
double
|
|
ScattDataTabular::calc_f(int gin, int gout, double mu)
|
|
{
|
|
double f;
|
|
if ((gout < gmin[gin]) || (gout > gmax[gin])) {
|
|
f = 0.;
|
|
} else {
|
|
// Find mu bin
|
|
int i_gout = gout - gmin[gin];
|
|
int imu;
|
|
if (mu == 1.) {
|
|
// use size -2 to have the index one before the end
|
|
imu = this->mu.size() - 2;
|
|
} else {
|
|
imu = std::floor((mu + 1.) / dmu + 1.) - 1;
|
|
}
|
|
|
|
double r = (mu - this->mu[imu]) / (this->mu[imu + 1] - this->mu[imu]);
|
|
f = (1. - r) * fmu[gin][i_gout][imu] + r * fmu[gin][i_gout][imu + 1];
|
|
}
|
|
return f;
|
|
}
|
|
|
|
//==============================================================================
|
|
|
|
void
|
|
ScattDataTabular::sample(int gin, int& gout, double& mu, double& wgt)
|
|
{
|
|
// Sample the outgoing energy using the base-class method
|
|
int i_gout;
|
|
sample_energy(gin, gout, i_gout);
|
|
|
|
// Determine the outgoing cosine bin
|
|
int NP = this->mu.size();
|
|
double xi = prn();
|
|
|
|
double c_k = dist[gin][i_gout][0];
|
|
int k;
|
|
for (k = 0; k < NP - 1; k++) {
|
|
double c_k1 = dist[gin][i_gout][k + 1];
|
|
if (xi < c_k1) break;
|
|
c_k = c_k1;
|
|
}
|
|
|
|
// Check to make sure k is <= NP - 1
|
|
k = std::min(k, NP - 2);
|
|
|
|
// Find the pdf values we want
|
|
double p0 = fmu[gin][i_gout][k];
|
|
double mu0 = this -> mu[k];
|
|
double p1 = fmu[gin][i_gout][k + 1];
|
|
double mu1 = this -> mu[k + 1];
|
|
|
|
if (p0 == p1) {
|
|
mu = mu0 + (xi - c_k) / p0;
|
|
} else {
|
|
double frac = (p1 - p0) / (mu1 - mu0);
|
|
mu = mu0 + (std::sqrt(std::max(0., p0 * p0 + 2. * frac * (xi - c_k)))
|
|
- p0) / frac;
|
|
}
|
|
|
|
if (mu < -1.) {
|
|
mu = -1.;
|
|
} else if (mu > 1.) {
|
|
mu = 1.;
|
|
}
|
|
|
|
// Update the weight to reflect neutron multiplicity
|
|
wgt *= mult[gin][i_gout];
|
|
}
|
|
|
|
//==============================================================================
|
|
|
|
double_3dvec
|
|
ScattDataTabular::get_matrix(int max_order)
|
|
{
|
|
// Get the sizes and initialize the data to 0
|
|
int groups = energy.size();
|
|
// We ignore the requested order for Histogram and Tabular representations
|
|
int order_dim = get_order();
|
|
double_3dvec matrix = double_3dvec(groups, double_2dvec(groups,
|
|
double_1dvec(order_dim, 0.)));
|
|
|
|
for (int gin = 0; gin < groups; gin++) {
|
|
for (int i_gout = 0; i_gout < energy[gin].size(); i_gout++) {
|
|
int gout = i_gout + gmin[gin];
|
|
for (int l = 0; l < order_dim; l++) {
|
|
matrix[gin][gout][l] = scattxs[gin] * energy[gin][i_gout] *
|
|
fmu[gin][i_gout][l];
|
|
}
|
|
}
|
|
}
|
|
return matrix;
|
|
}
|
|
|
|
//==============================================================================
|
|
|
|
void
|
|
ScattDataTabular::combine(const std::vector<ScattData*>& those_scatts,
|
|
const double_1dvec& scalars)
|
|
{
|
|
// Find the max order in the data set and make sure we can combine the sets
|
|
int max_order = those_scatts[0]->get_order();
|
|
for (int i = 0; i < those_scatts.size(); i++) {
|
|
// Lets also make sure these items are combineable
|
|
ScattDataTabular* that = dynamic_cast<ScattDataTabular*>(those_scatts[i]);
|
|
if (!that) {
|
|
fatal_error("Cannot combine the ScattData objects!");
|
|
}
|
|
if (max_order != that->get_order()) {
|
|
fatal_error("Cannot combine the ScattData objects!");
|
|
}
|
|
}
|
|
|
|
int groups = those_scatts[0] -> energy.size();
|
|
|
|
int_1dvec in_gmin(groups);
|
|
int_1dvec in_gmax(groups);
|
|
double_3dvec sparse_scatter(groups);
|
|
double_2dvec sparse_mult(groups);
|
|
|
|
// The rest of the steps do not depend on the type of angular representation
|
|
// so we use a base class method to sum up xs and create new energy and mult
|
|
// matrices
|
|
ScattData::base_combine(max_order, those_scatts, scalars, in_gmin, in_gmax,
|
|
sparse_mult, sparse_scatter);
|
|
|
|
// Got everything we need, store it.
|
|
init(in_gmin, in_gmax, sparse_mult, sparse_scatter);
|
|
}
|
|
|
|
//==============================================================================
|
|
// module-level methods
|
|
//==============================================================================
|
|
|
|
void
|
|
convert_legendre_to_tabular(ScattDataLegendre& leg, ScattDataTabular& tab,
|
|
int n_mu)
|
|
{
|
|
// See if the user wants us to figure out how many points to use
|
|
if (n_mu == C_NONE) {
|
|
// then we will use 2 pts if its P0, or the default if a higher order
|
|
// TODO use an error minimization algorithm that also picks n_mu
|
|
if (leg.get_order() == 0) {
|
|
n_mu = 2;
|
|
} else {
|
|
n_mu = DEFAULT_NMU;
|
|
}
|
|
}
|
|
|
|
tab.base_init(n_mu, leg.gmin, leg.gmax, leg.energy, leg.mult);
|
|
tab.scattxs = leg.scattxs;
|
|
|
|
// Build mu and dmu
|
|
tab.mu = double_1dvec(n_mu);
|
|
tab.dmu = 2. / (n_mu - 1);
|
|
tab.mu[0] = -1.;
|
|
for (int imu = 1; imu < n_mu - 1; imu++) {
|
|
tab.mu[imu] = -1. + imu * tab.dmu;
|
|
}
|
|
tab.mu[n_mu - 1] = 1.;
|
|
|
|
// Calculate f(mu) and integrate it so we can avoid rejection sampling
|
|
int groups = tab.energy.size();
|
|
tab.fmu.resize(groups);
|
|
for (int gin = 0; gin < groups; gin++) {
|
|
int num_groups = tab.gmax[gin] - tab.gmin[gin] + 1;
|
|
tab.fmu[gin].resize(num_groups);
|
|
for (int i_gout = 0; i_gout < num_groups; i_gout++) {
|
|
tab.fmu[gin][i_gout].resize(n_mu);
|
|
for (int imu = 0; imu < n_mu; imu++) {
|
|
tab.fmu[gin][i_gout][imu] =
|
|
evaluate_legendre_c(leg.dist[gin][i_gout].size() - 1,
|
|
leg.dist[gin][i_gout].data(), tab.mu[imu]);
|
|
}
|
|
|
|
// Ensure positivity
|
|
for (auto& val : tab.fmu[gin][i_gout]) {
|
|
if (val < 0.) val = 0.;
|
|
}
|
|
|
|
// Now re-normalize for numerical integration issues and to take care of
|
|
// the above negative fix-up. Also accrue the CDF
|
|
double norm = 0.;
|
|
tab.dist[gin][i_gout][0] = 0.;
|
|
for (int imu = 1; imu < n_mu; imu++) {
|
|
norm += 0.5 * tab.dmu * (tab.fmu[gin][i_gout][imu - 1] +
|
|
tab.fmu[gin][i_gout][imu]);
|
|
// incorporate to the CDF
|
|
tab.dist[gin][i_gout][imu] = norm;
|
|
}
|
|
|
|
// now do the normalization
|
|
if (norm > 0.) {
|
|
for (int imu = 0; imu < n_mu; imu++) {
|
|
tab.fmu[gin][i_gout][imu] /= norm;
|
|
tab.dist[gin][i_gout][imu] /= norm;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
}
|
|
|
|
} // namespace openmc
|