WMuNuCandidate.cc

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#include "AnalysisDataFormats/EWK/interface/WMuNuCandidate.h"
#include "DataFormats/TrackReco/interface/Track.h"
#include "CommonTools/CandUtils/interface/CandCombiner.h"
#include "CommonTools/CandUtils/interface/AddFourMomenta.h"

using namespace edm;
using namespace std;
using namespace reco;

WMuNuCandidate::WMuNuCandidate() {}

WMuNuCandidate::WMuNuCandidate(edm::Ptr<reco::Muon> muon, edm::Ptr<reco::MET> met) : muon_(muon), neutrino_(met) {
  addDaughter(*muon, "Muon");
  addDaughter(*met, "Met");
  AddFourMomenta addP4;
  addP4.set(*this);

  //WARNING: W Candidates 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 Candidate functions (.mass, .mt, .et, etc). They may not be what you are looking for :-).
}

WMuNuCandidate::~WMuNuCandidate() {}

double WMuNuCandidate::eT() const {
  double e_t = 0;
  e_t = muon_->pt() + neutrino_->pt();
  return e_t;
}

double WMuNuCandidate::massT() const {
  // Candidates have a mt() function which computes the tranverse mass from E & pz.
  // As MET does not have pz information... WMuNuCandidates have an alternative function to compute the mt quantity
  // used in the WMuNu Inclusive analysis just from px, py
  double wpx = px();
  double wpy = py();
  double mt = eT() * eT() - wpx * wpx - wpy * wpy;
  mt = (mt > 0) ? sqrt(mt) : 0;
  return mt;
}

double WMuNuCandidate::acop() const {
  // Acoplanarity between the muon and the MET
  Geom::Phi<double> deltaphi(daughter(0)->phi() - daughter(1)->phi());
  double acop = deltaphi.value();
  if (acop < 0)
    acop = -acop;
  acop = M_PI - acop;
  return acop;
}