Rivet analyses
Precise study of Z pT using novel phi* technique
Experiment: D0 (Tevatron Run 2)
Inspire ID: 871787
Status: VALIDATED
Authors: - Frank Siegert
References: - arXiv: 1010.0262
Beams: p- p+
Beam energies: (980.0, 980.0)GeV
Run details: - Inclusive Z/γ* production in both electron and muon channels. Cut on invariant lepton mass should be wider than 70 < mℓℓ < 110 GeV.
Using 7.3 pb−1 the distribution of the variable ϕ* is measured, which probes the same physical effects as the Z/γ* boson transverse momentum, but is less susceptible to the effects of experimental resolution and efficiency. Results are presented for both the di-electron and di-muon channel.
Source
code:D0_2010_I871787.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/FinalState.hh"
#include "Rivet/Projections/DileptonFinder.hh"
namespace Rivet {
/// Precise study of Z pT using novel phi* technique
class D0_2010_I871787 : public Analysis {
public:
RIVET_DEFAULT_ANALYSIS_CTOR(D0_2010_I871787);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
/// Initialise and register projections
FinalState fs;
Cut cuts_e = (Cuts::abseta < 1.1 || Cuts::absetaIn( 1.5, 3.0)) && Cuts::pT > 20*GeV;
DileptonFinder zfinder_ee(91.2*GeV, 0.2, cuts_e && Cuts::abspid == PID::ELECTRON, Cuts::massIn(70*GeV, 110*GeV));
declare(zfinder_ee, "zfinder_ee");
Cut cuts_m = Cuts::abseta < 2 && Cuts::pT > 15*GeV;
DileptonFinder zfinder_mm(91.2*GeV, 0.0, cuts_m && Cuts::abspid == PID::MUON, Cuts::massIn(70*GeV, 110*GeV));
declare(zfinder_mm, "zfinder_mm");
/// Book histograms here
book(_h_phistar_ee, {0., 1., 2., 10.}, {"d01-x01-y01", "d01-x01-y02", "d01-x01-y03"});
book(_h_phistar_mm, {0., 1., 2.}, {"d02-x01-y01", "d02-x01-y02"});
}
/// Perform the per-event analysis
void analyze(const Event& event) {
const DileptonFinder& zfinder_ee = apply<DileptonFinder>(event, "zfinder_ee");
if (zfinder_ee.bosons().size() == 1) {
Particles ee = zfinder_ee.constituents();
std::sort(ee.begin(), ee.end(), cmpMomByPt);
const FourMomentum& eminus = PID::charge3(ee[0].pid()) < 0 ? ee[0].momentum() : ee[1].momentum();
const FourMomentum& eplus = PID::charge3(ee[0].pid()) < 0 ? ee[1].momentum() : ee[0].momentum();
double phi_acop = M_PI - mapAngle0ToPi(eminus.phi() - eplus.phi());
double costhetastar = tanh((eminus.eta() - eplus.eta())/2);
double sin2thetastar = 1 - sqr(costhetastar);
if (sin2thetastar < 0) sin2thetastar = 0;
const double phistar = tan(phi_acop/2) * sqrt(sin2thetastar);
const FourMomentum& zmom = zfinder_ee.bosons()[0].momentum();
_h_phistar_ee->fill(zmom.rapidity(), phistar);
}
const DileptonFinder& zfinder_mm = apply<DileptonFinder>(event, "zfinder_mm");
if (zfinder_mm.bosons().size() == 1) {
Particles mm = zfinder_mm.constituents();
std::sort(mm.begin(), mm.end(), cmpMomByPt);
const FourMomentum& mminus = PID::charge3(mm[0].pid()) < 0 ? mm[0].momentum() : mm[1].momentum();
const FourMomentum& mplus = PID::charge3(mm[0].pid()) < 0 ? mm[1].momentum() : mm[0].momentum();
double phi_acop = M_PI - mapAngle0ToPi(mminus.phi() - mplus.phi());
double costhetastar = tanh((mminus.eta() - mplus.eta())/2);
double sin2thetastar = 1 - sqr(costhetastar);
if (sin2thetastar < 0) sin2thetastar = 0;
const double phistar = tan(phi_acop/2) * sqrt(sin2thetastar);
const FourMomentum& zmom = zfinder_mm.bosons()[0].momentum();
_h_phistar_mm->fill(zmom.rapidity(), phistar);
}
}
/// Normalise histograms etc., after the run
void finalize() {
normalize({_h_phistar_ee, _h_phistar_mm});
}
/// @}
private:
/// @name Histograms
/// @{
Histo1DGroupPtr _h_phistar_ee, _h_phistar_mm;
/// @}
};
RIVET_DECLARE_ALIASED_PLUGIN(D0_2010_I871787, D0_2010_S8821313);
}Aliases: - D0_2010_S8821313