G4INCLInvFInterpolationTable.cc

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//
// INCL++ intra-nuclear cascade model
// Alain Boudard, CEA-Saclay, France
// Joseph Cugnon, University of Liege, Belgium
// Jean-Christophe David, CEA-Saclay, France
// Pekka Kaitaniemi, CEA-Saclay, France, and Helsinki Institute of Physics, Finland
// Sylvie Leray, CEA-Saclay, France
// Davide Mancusi, CEA-Saclay, France
//
#define INCLXX_IN_GEANT4_MODE 1
 
#include "globals.hh"
 
/** \file G4INCLInvFInterpolationTable.cc
 * \brief Simple interpolation table for the inverse of a IFunction1D functor
 *
 * \date 17 July 2012
 * \author Davide Mancusi
 */
 
// #include <cassert>
#include <algorithm>
#include <functional>
#include "G4INCLInvFInterpolationTable.hh"
 
namespace G4INCL {
 
  InvFInterpolationTable::InvFInterpolationTable(IFunction1D const &f, const unsigned int nNodes) {
// assert(nNodes>2);
 
    const G4double x0 = f.getXMinimum();
    const G4double x1 = f.getXMaximum();
 
    // Build the nodes
    G4double last = f(x0);
    InterpolationNode firstNode(last, x0, 0.);
    nodes.push_back(firstNode);
//  G4int skippedNodes = 0;
    for(unsigned i = 1; i < nNodes; i++) {
      const G4double xi = x0 + i*(x1-x0)/((G4double)(nNodes-1));
      // Make sure that the x vector is sorted (corresponding to a monotonous
      // function)
      const G4double value = f(xi);
      if(value <= last) {
//      ++skippedNodes;
        continue;
      }
      InterpolationNode node(value, xi, 0.);
      nodes.push_back(node);
      last = value;
    }
 
// assert(nNodes==nodes.size()+skippedNodes);
 
    // Initialise the "derivative" values
    initDerivatives();
  }
 
}