Rivet analyses
χc2 decays to K+K−π0, KS0K±π∓ and π+π−π0
Experiment: BESIII (BEPC)
Inspire ID: 1505590
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - Phys.Rev.D 96 (2017) 11, 111102
Beams: * *
Beam energies: ANY
Run details: - Any process producing chi_c2
Mass distributions in χc2 decays to K+K−π0, KS0K±π∓ and π+π−π0. The data was read from the plots in the paper and is not corrected for efficiency and acceptance.
Source
code:BESIII_2017_I1505590.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/DecayedParticles.hh"
#include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief chi_c2 decays
class BESIII_2017_I1505590 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(BESIII_2017_I1505590);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// projections
UnstableParticles ufs = UnstableParticles(Cuts::pid == 445);
declare(ufs, "UFS");
DecayedParticles chi(ufs);
chi.addStable(PID::PI0);
chi.addStable(PID::K0S);
declare(chi, "chi");
// histograms
for (unsigned int ix = 0; ix < 4; ++ix) {
if (ix < 2) book(_h[ix], 1, 1, 1 + ix);
book(_h[2 + ix], 2, 1, 1 + ix);
}
}
/// Perform the per-event analysis
void analyze(const Event& event) {
DecayedParticles chi = apply<DecayedParticles>(event, "chi");
// loop over particles
for (unsigned int ix = 0; ix < chi.decaying().size(); ++ix) {
int sign = 1;
// K+ K- pi0
if (chi.modeMatches(ix, 3, mode1)) {
const Particle& Kp = chi.decayProducts()[ix].at(321)[0];
const Particle& Km = chi.decayProducts()[ix].at(-321)[0];
const Particle& pi0 = chi.decayProducts()[ix].at(111)[0];
_h[0]->fill((Kp.mom() + pi0.mom()).mass() / GeV);
_h[0]->fill((Km.mom() + pi0.mom()).mass() / GeV);
_h[1]->fill((Kp.mom() + Km.mom()).mass() / GeV);
continue;
}
// pi+ pi- pi0
else if (chi.modeMatches(ix, 3, mode3)) {
const Particle& pip = chi.decayProducts()[ix].at(211)[0];
const Particle& pim = chi.decayProducts()[ix].at(-211)[0];
const Particle& pi0 = chi.decayProducts()[ix].at(111)[0];
_h[5]->fill((pip.mom() + pi0.mom()).mass() / GeV);
_h[5]->fill((pim.mom() + pi0.mom()).mass() / GeV);
continue;
}
else if (chi.modeMatches(ix, 3, mode2)) {
sign = 1;
}
else if (chi.modeMatches(ix, 3, mode2CC)) {
sign = -1;
}
else {
continue;
}
const Particle& KS0 = chi.decayProducts()[ix].at(310)[0];
const Particle& Kp = chi.decayProducts()[ix].at(sign * 321)[0];
const Particle& pim = chi.decayProducts()[ix].at(-sign * 211)[0];
_h[2]->fill((Kp.mom() + pim.mom()).mass() / GeV);
_h[3]->fill((KS0.mom() + pim.mom()).mass() / GeV);
_h[4]->fill((KS0.mom() + Kp.mom()).mass() / GeV);
}
}
/// Normalise histograms etc., after the run
void finalize() {
normalize(_h, 1.0, false);
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h[6];
const map<PdgId, unsigned int> mode1 = {{321, 1}, {-321, 1}, {111, 1}};
const map<PdgId, unsigned int> mode2 = {{310, 1}, {321, 1}, {-211, 1}};
const map<PdgId, unsigned int> mode2CC = {{310, 1}, {-321, 1}, {211, 1}};
const map<PdgId, unsigned int> mode3 = {{211, 1}, {-211, 1}, {111, 1}};
/// @}
};
RIVET_DECLARE_PLUGIN(BESIII_2017_I1505590);
}