Rivet analyses
Zyy cross-section measurement at 13 TeV
Experiment: ATLAS (LHC)
Inspire ID: 2593322
Status: VALIDATED
Authors: - Philipp Ott - Daniel Lewis
References: - arXiv: 2211.14171
Beams: p+ p+
Beam energies: (6500.0, 6500.0)GeV
Run details: - pp -> lly at 13 TeV
Cross-sections for the production of a Z boson in association with two photons are measured in proton-proton collisions at a centre-of-mass energy of 13 TeV. The data used correspond to an integrated luminosity of 139 fb−1 recorded by the ATLAS experiment during Run 2 of the LHC. The measurements use the electron and muon decay channels of the Z boson, and a fiducial phase-space region where the photons are not radiated from the leptons. The integrated Z( → ℓℓ)γγ cross-section is measured with a precision of 12% and differential cross-sections are measured as a function of six kinematic variables of the Zγγ system. The data are compared with predictions from MC event generators which are accurate to up to next-to-leading order in QCD. The cross-section measurements are used to set limits on the coupling strengths of dimension-8 operators in the framework of an effective field theory.
Source
code:ATLAS_2022_I2593322.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/FinalState.hh"
#include "Rivet/Projections/LeptonFinder.hh"
#include "Rivet/Projections/PromptFinalState.hh"
#include "Rivet/Projections/VetoedFinalState.hh"
#include "Rivet/Projections/VisibleFinalState.hh"
#include "Rivet/Projections/IdentifiedFinalState.hh"
namespace Rivet {
/// @brief ATLAS 13 TeV Z(->ll)yy analysis
class ATLAS_2022_I2593322 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(ATLAS_2022_I2593322);
/// @name Analysis methods
///@{
/// Book histograms and initialise projections before the run
void init() {
// Prompt photons
const Cut photoncut = Cuts::abspid == PID::PHOTON && Cuts::pT > 20*GeV && Cuts::abseta < 2.37;
PromptFinalState photon_fs(photoncut);
declare(photon_fs, "Photons");
// Prompt leptons
const PromptFinalState bareelectron_fs = Cuts::abspid == PID::ELECTRON;
const PromptFinalState baremuon_fs = Cuts::abspid == PID::MUON;
// Dressed leptons
const IdentifiedFinalState allphoton_fs(PID::PHOTON); // photons used for lepton dressing
const Cut leptoncut = Cuts::pT > 20*GeV && Cuts::abseta < 2.47;
const LeptonFinder dressedelectron_fs(bareelectron_fs, allphoton_fs, 0.1, leptoncut);
const LeptonFinder dressedmuon_fs(baremuon_fs, allphoton_fs, 0.1, leptoncut);
declare(dressedelectron_fs, "Electrons");
declare(dressedmuon_fs, "Muons");
IdentifiedFinalState neutrinos;
neutrinos.acceptNeutrinos();
// FS for photon isolation
FinalState all_fs;
VetoedFinalState veto_fs(all_fs);
veto_fs.addVetoOnThisFinalState(photon_fs);
veto_fs.addVetoOnThisFinalState(dressedmuon_fs);
veto_fs.addVetoOnThisFinalState(neutrinos);
declare(veto_fs, "vetoFS");
// book histograms
book(_h["y1_pt"], 2, 1, 1);
book(_h["y2_pt"], 3, 1, 1);
book(_h["ll_pt"], 4, 1, 1);
book(_h["llyy_pt"], 5, 1, 1);
book(_h["yy_m"], 6, 1, 1);
book(_h["llyy_m"], 7, 1, 1);
}
/// Perform the per-event analysis
void analyze(const Event& event) {
DressedLeptons electrons = apply<LeptonFinder>(event, "Electrons").dressedLeptons();
DressedLeptons muons = apply<LeptonFinder>(event, "Muons").dressedLeptons();
const Particles& photons = apply<PromptFinalState>(event, "Photons").particlesByPt();
if ( (electrons.size() < 2 && muons.size() < 2) ) vetoEvent;
if ( photons.size() < 2 ) vetoEvent;
DressedLepton *lep_1, *lep_2;
if (muons.size() >= 2){
if (muons[0].pT()/GeV < 30) vetoEvent;
lep_1 = &muons[0];
lep_2 = &muons[1];
}
else{
if (electrons[0].pT()/GeV < 30) vetoEvent;
lep_1 = &electrons[0];
lep_2 = &electrons[1];
}
if ( (lep_1->charge() == lep_2->charge()) || (lep_1->abspid() != lep_2->abspid()) ) vetoEvent;
Particles veto_particles = apply<VetoedFinalState>(event, "vetoFS").particles();
Particles selPhotons;
for (size_t i = 0; i < photons.size(); ++i){
if ( deltaR(photons[i], *lep_1) < 0.4 ) continue;
if ( deltaR(photons[i], *lep_2) < 0.4 ) continue;
double coneEnergy = 0;
for (const Particle &p : veto_particles){
if ( deltaR(photons[i], p) < 0.2 ) coneEnergy += p.Et();
}
if (coneEnergy/photons[i].Et() > 0.07) continue;
selPhotons.push_back(photons[i]);
}
if (selPhotons.size() < 2) vetoEvent;
if (deltaR(selPhotons[0], selPhotons[1]) < 0.4) vetoEvent;
if ( (lep_1->momentum() + lep_2->momentum()).mass()/GeV < 40 ) vetoEvent;
FourMomentum ll_p4 = lep_1->mom()+lep_2->mom();
const double m_ll = ll_p4.mass();
const bool lly0 = (ll_p4+selPhotons[0].mom()).mass() > (ll_p4+selPhotons[1].mom()).mass();
const double m_ll_y = lly0? (ll_p4+selPhotons[1].mom()).mass() : (ll_p4+selPhotons[0].mom()).mass();
if ( (m_ll + m_ll_y) < 182*GeV) vetoEvent;
FourMomentum yy_p4 = selPhotons[0].momentum()+selPhotons[1].momentum();
_h["y1_pt"]->fill(selPhotons[0].pt()/GeV);
_h["y2_pt"]->fill(selPhotons[1].pt()/GeV);
_h["ll_pt"]->fill(ll_p4.pt()/GeV);
_h["llyy_pt"]->fill( (ll_p4+yy_p4).pt()/GeV );
_h["yy_m"]->fill(yy_p4.mass()/GeV);
_h["llyy_m"]->fill( (ll_p4+yy_p4).mass()/GeV );
}
void finalize() {
const double sf = crossSection()/femtobarn/sumW();
scale(_h, sf);
}
///@}
/// @name Histograms
///@{
map<string, Histo1DPtr> _h;
///@}
};
RIVET_DECLARE_PLUGIN(ATLAS_2022_I2593322);
}