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// This software was developed by Lawrence Livermore National Laboratory.
//
// Redistribution and use in source and binary forms, with or without
// modification, are permitted provided that the following conditions are met:
//
// 1. Redistributions of source code must retain the above copyright notice,
//   this list of conditions and the following disclaimer.
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// Copyright (c) 2006 The Regents of the University of California.
// All rights reserved.
// UCRL-CODE-224807
//
//
//

#include <cmath>
#include "G4Exp.hh"
#include "G4Log.hh"
#include "G4fissionEvent.hh"

#define TWOPI 6.283185307
#define SQRT2 1.414213562
#define BSHIFT -0.43287
#define WIDTH 1.079

G4double G4fissionEvent::G4SmpTerrell(G4double nubar) {
/*
  Description
    Sample Fission Number from Terrell's modified Gaussian distribution

    method uses Red Cullen's algoritm UCRL-TR-222526
*/

/*
  Input
    nubar    - average number of neutrons per fission
  Output
    G4SmpTerrell  - sampled multiplicity
    
*/

  G4double width;
  G4double temp1, temp2, expo, cshift;
  G4double rw, theta, sampleg;


  if (nubar < WIDTH) {
    std::ostringstream o;
    o << nubar;
    const std::string& errMsg = "fission nubar out of range, nubar=" + o.str();
    G4fissionerr(6, "SmpTerrell", errMsg);
  }

  width = SQRT2 * WIDTH;
  temp1 = nubar + 0.5;
  temp2 = temp1/width;
  temp2 *= temp2;
  expo = G4Exp(-temp2);
  cshift = temp1 + BSHIFT * WIDTH * expo/(1. - expo);

  G4int icounter = 0;
  G4int icounter_max = 1024;
  do {
    rw = std::sqrt(-G4Log(fisslibrng()));
    theta = TWOPI * fisslibrng();
    sampleg = width * rw * std::cos(theta) + cshift;
    icounter++;
    if ( icounter > icounter_max ) { 
      G4cout << "Loop-counter exceeded the threshold value at " << __LINE__ << "th line of " << __FILE__ << "." << G4endl;
      break;
    }
  } while (sampleg < 0.0);
  // Loop checking, 11.03.2015, T. Koi

  return std::floor(sampleg);
}
