Rivet analyses
Analysis of ψ(2S) → γχc2 decays using χc2 → γγ
Experiment: BESIII (BEPC)
Inspire ID: 1624548
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - Phys.Rev.D 96 (2017) 9, 092007
Beams: e- e+
Beam energies: (1.8, 1.8)GeV
Run details: - e+e- > psi(2S)
Analysis of the angular distribution of the photons and leptons produced in e+e− → ψ(2S) → γχc2 followed by χc2 → γγ. Gives information about the decay and is useful for testing correlations in charmonium decays. N.B. the data was read from the figures in the paper and is not corrected and should only be used qualatively.
Source
code:BESIII_2017_I1624548.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/Beam.hh"
#include "Rivet/Projections/FinalState.hh"
#include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief psi(2S) -> gamma chi_c1,2
class BESIII_2017_I1624548 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(BESIII_2017_I1624548);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// Initialise and register projections
declare(Beam(), "Beams");
declare(UnstableParticles(Cuts::pid==445), "UFS");
declare(FinalState(), "FS");
for(unsigned int ix=0;ix<3;++ix)
book(_h[ix],1,1,1+ix);
}
void findChildren(const Particle & p,map<long,int> & nRes, int &ncount) {
for( const Particle &child : p.children()) {
if(child.children().empty()) {
nRes[child.pid()]-=1;
--ncount;
}
else
findChildren(child,nRes,ncount);
}
}
/// Perform the per-event analysis
void analyze(const Event& event) {
// get the axis, direction of incoming electron
const ParticlePair& beams = apply<Beam>(event, "Beams").beams();
Vector3 axis;
if(beams.first.pid()>0)
axis = beams.first .momentum().p3().unit();
else
axis = beams.second.momentum().p3().unit();
// types of final state particles
const FinalState& fs = apply<FinalState>(event, "FS");
map<long,int> nCount;
int ntotal(0);
for (const Particle& p : fs.particles()) {
nCount[p.pid()] += 1;
++ntotal;
}
// loop over chi_c states
Particle chi;
bool matched = false;
const UnstableParticles & ufs = apply<UnstableParticles>(event, "UFS");
for (const Particle& p : ufs.particles()) {
if(p.children().empty()) continue;
map<long,int> nRes=nCount;
int ncount = ntotal;
findChildren(p,nRes,ncount);
if(ncount==1) {
matched = true;
for(auto const & val : nRes) {
if(val.first==PID::PHOTON) {
if(val.second!=1) {
matched = false;
break;
}
}
else if(val.second!=0) {
matched = false;
break;
}
}
if(matched) {
chi=p;
break;
}
}
}
if(!matched) vetoEvent;
// have chi_c find psi2S
if(chi.parents().empty() || chi.children().size()!=2) vetoEvent;
Particle psi2S = chi.parents()[0];
if(psi2S.pid()!=100443 || psi2S.children().size()!=2) vetoEvent;
// then the first photon
Particle gamma1;
if(psi2S.children()[0].pid()==PID::PHOTON)
gamma1 = psi2S.children()[0];
else if(psi2S.children()[1].pid()==PID::PHOTON)
gamma1 = psi2S.children()[1];
else
vetoEvent;
// and second photon
Particle gamma2;
if(chi.children()[0].pid()==PID::PHOTON &&
chi.children()[1].pid()==PID::PHOTON) {
gamma2 = chi.children()[0];
}
else
vetoEvent;
// first angle of gamma1 w.r.t beam
_h[0]->fill(axis.dot(gamma1.momentum().p3().unit()));
// axis in the chi frame
LorentzTransform boost1 = LorentzTransform::mkFrameTransformFromBeta(chi.momentum().betaVec());
Vector3 e1z = gamma1.momentum().p3().unit();
Vector3 e1y = e1z.cross(axis).unit();
Vector3 e1x = e1y.cross(e1z).unit();
// cos theta_2 and phi 2 distributions
FourMomentum pGamma2 = boost1.transform(gamma2.momentum());
Vector3 axis1 = pGamma2.p3().unit();
_h[1]->fill(e1z.dot(axis1));
double phi2 = atan2(e1y.dot(axis1),e1x.dot(axis1));
if(phi2<0) phi2+=2.*M_PI;
_h[2]->fill(phi2);
}
/// Normalise histograms etc., after the run
void finalize() {
for(unsigned int ix=0;ix<3;++ix) {
normalize(_h[ix],1.,false);
}
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h[3];
/// @}
};
RIVET_DECLARE_PLUGIN(BESIII_2017_I1624548);
}