WMuNuCandidatePtr.cc

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#include "AnalysisDataFormats/EWK/interface/WMuNuCandidatePtr.h"
#include "CommonTools/CandUtils/interface/CandCombiner.h"
#include "CommonTools/CandUtils/interface/AddFourMomenta.h"
#include "DataFormats/TrackReco/interface/Track.h"
 
using namespace edm;
using namespace std;
using namespace reco;
 
WMuNuCandidatePtr::WMuNuCandidatePtr() {}
 
WMuNuCandidatePtr::WMuNuCandidatePtr(const reco::CandidatePtr muon, const reco::CandidatePtr met)
    : muon_(muon), neutrino_(met) {
  addDaughter(muon_);
  addDaughter(neutrino_);
  AddFourMomenta addP4;
  addP4.set(*this);
  cout << "WCandidatePtr Created   Wpx=" << muon_->px() << " + " << neutrino_->px() << " ?= " << this->px() << endl;
  //WARNING: W CandidatePtrs combine the information from a Muon with the (px,py) information of the MET as the Neutrino
  // --> There is no Pz information!!!!
  // Be very careful when using the default CandidatePtr functions (.mass, .mt, .et, etc). They may not be what you are looking for :-).
}
 
WMuNuCandidatePtr::~WMuNuCandidatePtr() {}
 
double WMuNuCandidatePtr::eT() const {
  double e_t = 0;
  e_t = muon_->pt() + neutrino_->pt();
  return e_t;
}
 
double WMuNuCandidatePtr::massT() const {
  // CandidatePtrs have a mt() function which computes the tranverse mass from E & pz.
  // As MET does not have pz information... WMuNuCandidatePtrs have an alternative function to compute the mt quantity
  // used in the WMuNu Inclusive analysis just from px, py
  double wpx = muon_->px() + neutrino_->px();
  double wpy = muon_->py() + neutrino_->py();
  double mt = eT() * eT() - wpx * wpx - wpy * wpy;
  mt = (mt > 0) ? sqrt(mt) : 0;
  return mt;
}
 
double WMuNuCandidatePtr::acop() const {
  // Acoplanarity between the muon and the MET
  Geom::Phi<double> deltaphi(muon_->phi() - neutrino_->phi());
  double acop = deltaphi.value();
  if (acop < 0)
    acop = -acop;
  acop = M_PI - acop;
  return acop;
}