Top_Decaykin.cc

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//
//
// File: src/Top_Decaykin.cc
// Purpose: Calculate some kinematic quantities for ttbar events.
// Created: Jul, 2000, sss, based on run 1 mass analysis code.
//
// CMSSW File      : src/Top_Decaykin.cc
// Original Author : Scott Stuart Snyder <snyder@bnl.gov> for D0
// Imported to CMSSW by Haryo Sumowidagdo <Suharyo.Sumowidagdo@cern.ch>
//
 
#include "TopQuarkAnalysis/TopHitFit/interface/Top_Decaykin.h"
#include "TopQuarkAnalysis/TopHitFit/interface/Lepjets_Event.h"
#include "TopQuarkAnalysis/TopHitFit/interface/fourvec.h"
#include <cmath>
#include <algorithm>
#include <ostream>
 
using std::abs;
using std::ostream;
using std::sqrt;
using std::swap;
 
namespace hitfit {
 
  namespace {
 
    Fourvec leptons(const Lepjets_Event& ev)
    //
    // Purpose: Sum all leptons in EV.
    //
    // Inputs:
    //   ev -          The event.
    //
    // Returns:
    //   The sum of all leptons in EV.
    //
    {
      return (ev.sum(lepton_label) + ev.sum(electron_label) + ev.sum(muon_label));
    }
 
  }  // unnamed namespace
 
  bool Top_Decaykin::solve_nu_tmass(const Lepjets_Event& ev, double tmass, double& nuz1, double& nuz2)
  //
  // Purpose: Solve for the neutrino longitudinal z-momentum that makes
  //          the leptonic top have mass TMASS.
  //
  // Inputs:
  //   ev -          The event to solve.
  //   tmass -       The desired top mass.
  //
  // Outputs:
  //   nuz1 -        First solution (smaller absolute value).
  //   nuz2 -        Second solution.
  //
  // Returns:
  //   True if there was a real solution.  False if there were only
  //   imaginary solutions.  (In that case, we just set the imaginary
  //   part to zero.)
  //
  {
    bool discrim_flag = true;
 
    const Fourvec& vnu = ev.met();
    Fourvec cprime = leptons(ev) + ev.sum(lepb_label);
    double alpha1 = tmass * tmass - cprime.m2();
    double a = 2 * 4 * (cprime.z() * cprime.z() - cprime.e() * cprime.e());
    double alpha = alpha1 + 2 * (cprime.x() * vnu.x() + cprime.y() * vnu.y());
    double b = 4 * alpha * cprime.z();
    double c = alpha * alpha - 4 * cprime.e() * cprime.e() * vnu.vect().perp2();
    double d = b * b - 2 * a * c;
    if (d < 0) {
      discrim_flag = false;
      d = 0;
    }
 
    double dd = sqrt(d);
    nuz1 = (-b + dd) / a;
    nuz2 = (-b - dd) / a;
    if (abs(nuz1) > abs(nuz2))
      swap(nuz1, nuz2);
 
    return discrim_flag;
  }
 
  bool Top_Decaykin::solve_nu_tmass(
      const Lepjets_Event& ev, double tmass, double& re_nuz1, double& im_nuz1, double& re_nuz2, double& im_nuz2)
  //
  // Purpose: Solve for the neutrino longitudinal z-momentum that makes
  //          the leptonic top have mass TMASS, including the imaginary
  //          component of the z-component of the neutrino'somentum.
  //
  // Inputs:
  //   ev -          The event to solve.
  //   tmass -       The desired top mass.
  //
  // Outputs:
  //   re_nuz1 -     Real component of the first solution.
  //   im_nuz1 -     Imaginary component of the first solution (in the lower half of
  //                 the complex plane).
  //   re_nuz2 -     Real component of the second solution.
  //   im_nuz2 -     Imaginary component of the second solution (in the upper half of
  //                 the complex plane).
  //
  // Returns:
  //   True if there was a real solution.  False if there were only
  //   complex solutions.
  //
  {
    bool discrim_flag = true;
 
    const Fourvec& vnu = ev.met();
    Fourvec cprime = leptons(ev) + ev.sum(lepb_label);
    double alpha1 = tmass * tmass - cprime.m2();
    double a = 2 * 4 * (cprime.z() * cprime.z() - cprime.e() * cprime.e());
    // Haryo's note: Here a is equivalent to '2a' in the quadratic
    // equation ax^2 + bx + c = 0
    double alpha = alpha1 + 2 * (cprime.x() * vnu.x() + cprime.y() * vnu.y());
    double b = 4 * alpha * cprime.z();
    double c = alpha * alpha - 4 * cprime.e() * cprime.e() * vnu.vect().perp2();
    double d = b * b - 2 * a * c;
    if (d < 0) {
      discrim_flag = false;
    }
 
    if (discrim_flag) {
      re_nuz1 = (-b + sqrt(d)) / a;
      im_nuz1 = 0;
      re_nuz2 = (-b - sqrt(d)) / a;
      im_nuz2 = 0;
      if (abs(re_nuz1) > abs(re_nuz2)) {
        swap(re_nuz1, re_nuz2);
      }
 
    } else {
      // Take absolute value of the imaginary component of nuz, in case
      // a is negative, before multiplying by +1 or -1 to get the upper-half
      // or lower-half imaginary value.
      re_nuz1 = -b / a;
      im_nuz1 = -fabs(sqrt(-d) / a);
      re_nuz2 = -b / a;
      im_nuz2 = fabs(sqrt(-d) / a);
    }
 
    return discrim_flag;
  }
 
  bool Top_Decaykin::solve_nu(const Lepjets_Event& ev, double wmass, double& nuz1, double& nuz2)
  //
  // Purpose: Solve for the neutrino longitudinal z-momentum that makes
  //          the leptonic W have mass WMASS.
  //
  // Inputs:
  //   ev -          The event to solve.
  //   wmass -       The desired W mass.
  //
  // Outputs:
  //   nuz1 -        First solution (smaller absolute value).
  //   nuz2 -        Second solution.
  //
  // Returns:
  //   True if there was a real solution.  False if there were only
  //   imaginary solutions.  (In that case, we just set the imaginary
  //   part to zero.)
  //
  {
    bool discrim_flag = true;
 
    const Fourvec& vnu = ev.met();
    Fourvec vlep = leptons(ev);
 
    double x = vlep.x() * vnu.x() + vlep.y() * vnu.y() + wmass * wmass / 2;
    double a = vlep.z() * vlep.z() - vlep.e() * vlep.e();
    double b = 2 * x * vlep.z();
    double c = x * x - vnu.perp2() * vlep.e() * vlep.e();
 
    double d = b * b - 4 * a * c;
    if (d < 0) {
      d = 0;
      discrim_flag = false;
    }
 
    nuz1 = (-b + sqrt(d)) / 2 / a;
    nuz2 = (-b - sqrt(d)) / 2 / a;
    if (abs(nuz1) > abs(nuz2))
      swap(nuz1, nuz2);
 
    return discrim_flag;
  }
 
  bool Top_Decaykin::solve_nu(
      const Lepjets_Event& ev, double wmass, double& re_nuz1, double& im_nuz1, double& re_nuz2, double& im_nuz2)
  //
  // Purpose: Solve for the neutrino longitudinal z-momentum that makes
  //          the leptonic W have mass WMASS, including the imaginary
  //          component of the z-component of the neutrino'somentum.
  //
  // Inputs:
  //   ev -          The event to solve.
  //   wmass -       The desired W mass.
  //
  // Outputs:
  //   re_nuz1 -     Real component of the first solution.
  //   im_nuz1 -     Imaginary component of the first solution  (in the lower half of
  //                 the complex plane).
  //   re_nuz2 -     Real component of the second solution.
  //   im_nuz2 -     Imaginary component of the second solution  (in the upper half of
  //                 the complex plane).
  //
  // Returns:
  //   True if there was a real solution.  False if there were only
  //   complex solutions.
  //x
  {
    bool discrim_flag = true;
 
    const Fourvec& vnu = ev.met();
    Fourvec vlep = leptons(ev);
 
    double x = vlep.x() * vnu.x() + vlep.y() * vnu.y() + wmass * wmass / 2;
    double a = vlep.z() * vlep.z() - vlep.e() * vlep.e();
    double b = 2 * x * vlep.z();
    double c = x * x - vnu.perp2() * vlep.e() * vlep.e();
 
    double d = b * b - 4 * a * c;
    if (d < 0) {
      discrim_flag = false;
    }
 
    if (discrim_flag) {
      re_nuz1 = (-b + sqrt(d)) / 2 / a;
      im_nuz1 = 0.0;
      re_nuz2 = (-b - sqrt(d)) / 2 / a;
      im_nuz2 = 0.0;
      if (fabs(re_nuz1) > fabs(re_nuz2)) {
        swap(re_nuz1, re_nuz2);
      }
 
    } else {
      // Take absolute value of the imaginary component of nuz, in case
      // a is negative, before multiplying by +1 or -1 to get the upper-half
      // or lower-half imaginary value.
 
      re_nuz1 = -b / 2 / a;
      im_nuz1 = -fabs(sqrt(-d) / a);
      re_nuz2 = -b / 2 / a;
      im_nuz2 = fabs(sqrt(-d) / a);
    }
 
    return discrim_flag;
  }
 
  Fourvec Top_Decaykin::hadw(const Lepjets_Event& ev)
  //
  // Purpose: Sum up the appropriate 4-vectors to find the hadronic W.
  //
  // Inputs:
  //   ev -          The event.
  //
  // Returns:
  //   The hadronic W.
  //
  {
    return (ev.sum(hadw1_label) + ev.sum(hadw2_label));
  }
 
  Fourvec Top_Decaykin::hadw1(const Lepjets_Event& ev)
  //
  // Purpose:
  //
  // Inputs:
  //   ev -          The event.
  //
  // Returns:
  //   The higher-pT hadronic jet from W
  //
  {
    return ev.sum(hadw1_label);
  }
 
  Fourvec Top_Decaykin::hadw2(const Lepjets_Event& ev)
  //
  // Purpose:
  //
  // Inputs:
  //   ev -          The event.
  //
  // Returns:
  //   The lower-pT hadronic jet from W
  //
  //
  {
    return ev.sum(hadw2_label);
  }
 
  Fourvec Top_Decaykin::lepw(const Lepjets_Event& ev)
  //
  // Purpose: Sum up the appropriate 4-vectors to find the leptonic W.
  //
  // Inputs:
  //   ev -          The event.
  //
  // Returns:
  //   The leptonic W.
  //
  {
    return (leptons(ev) + ev.met());
  }
 
  Fourvec Top_Decaykin::hadt(const Lepjets_Event& ev)
  //
  // Purpose: Sum up the appropriate 4-vectors to find the hadronic t.
  //
  // Inputs:
  //   ev -          The event.
  //
  // Returns:
  //   The hadronic t.
  //
  {
    return (ev.sum(hadb_label) + hadw(ev));
  }
 
  Fourvec Top_Decaykin::lept(const Lepjets_Event& ev)
  //
  // Purpose: Sum up the appropriate 4-vectors to find the leptonic t.
  //
  // Inputs:
  //   ev -          The event.
  //
  // Returns:
  //   The leptonic t.
  //
  {
    return (ev.sum(lepb_label) + lepw(ev));
  }
 
  ostream& Top_Decaykin::dump_ev(std::ostream& s, const Lepjets_Event& ev)
  //
  // Purpose: Print kinematic information for EV.
  //
  // Inputs:
  //   s -           The stream to which to write.
  //   ev -          The event to dump.
  //
  // Returns:
  //   The stream S.
  //
  {
    s << ev;
    Fourvec p;
 
    p = lepw(ev);
    s << "lepw " << p << " " << p.m() << "\n";
    p = lept(ev);
    s << "lept " << p << " " << p.m() << "\n";
    p = hadw(ev);
    s << "hadw " << p << " " << p.m() << "\n";
    p = hadt(ev);
    s << "hadt " << p << " " << p.m() << "\n";
 
    return s;
  }
 
  double Top_Decaykin::cos_theta_star(const Fourvec& fermion, const Fourvec& W, const Fourvec& top)
  //
  // Purpose: Calculate cos theta star in top decay
  //
  // Inputs:
  //   fermion -     The four momentum of fermion from W
  //   W -           The four momentum of W from top
  //   top -         The four momentum of top
  // Returns:
  //   cos theta star
  //
  {
    if (W.isLightlike() || W.isSpacelike()) {
      return 100.0;
    }
 
    CLHEP::HepBoost BoostWCM(W.findBoostToCM());
 
    CLHEP::Hep3Vector boost_v3fermion = BoostWCM(fermion).vect();
    CLHEP::Hep3Vector boost_v3top = BoostWCM(top).vect();
 
    double costhetastar = boost_v3fermion.cosTheta(-boost_v3top);
 
    return costhetastar;
  }
 
  double Top_Decaykin::cos_theta_star(const Lepjets_Event& ev)
  //
  // Purpose: Calculate lepton cos theta star in top decay
  //
  // Inputs:
  //   ev -          A lepton+jets event
  // Returns:
  //   cos theta star of lepton
  //
  {
    return cos_theta_star(leptons(ev), lepw(ev), lept(ev));
  }
 
  double Top_Decaykin::cos_theta_star_lept(const Lepjets_Event& ev)
  //
  // Purpose: Calculate lepton cos theta star in top decay
  //
  // Inputs:
  //   ev -          A lepton+jets event
  // Returns:
  //   cos theta star of lepton
  //
  {
    return cos_theta_star(ev);
  }
 
  double Top_Decaykin::cos_theta_star_hadt(const Lepjets_Event& ev)
  //
  // Purpose: Calculate absolute value of cos theta star of
  //          one of the hadronic W jet from hadronic top.
  //
  // Inputs:
  //   ev -          A lepton+jets event
  // Returns:
  //   absolute value of cos theta star
  //
  {
    return fabs(cos_theta_star(hadw1(ev), hadw(ev), hadt(ev)));
  }
 
}  // namespace hitfit