Rivet analyses
Kinematic distributions in the decay η → π+π−π0 and η(′) → π0π0π0
Experiment: BESIII (BEPC)
Inspire ID: 1376484
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - Phys.Rev.D 92 (2015) 012014
Beams: * *
Beam energies: ANY
Run details: - Any process producing eta/etaprime mesons
Measurement of kinematic distributions in the decays η → π+π−π0 and η(′) → π0π0π0. The data was read from the plots in the paper and the backgrounds subtract in the η′ decays.
Source
code:BESIII_2015_I1376484.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/DecayedParticles.hh"
#include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief eta -> pi+pi-pi0 and eta' -> pi0pi0pi0$
class BESIII_2015_I1376484 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(BESIII_2015_I1376484);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// Initialise and register projections
UnstableParticles ufs = UnstableParticles(Cuts::pid == PID::ETA or Cuts::pid == PID::ETAPRIME);
declare(ufs, "UFS");
DecayedParticles ETA(ufs);
ETA.addStable(PID::PI0);
ETA.addStable(PID::K0S);
ETA.addStable(PID::ETA);
declare(ETA, "ETA");
for (unsigned int ix = 0; ix < 2; ++ix) {
book(_h[ix], 1, 1, 1 + ix);
book(_h[ix + 2], 2 + ix, 1, 1);
}
}
/// Perform the per-event analysis
void analyze(const Event& event) {
static const map<PdgId, unsigned int>& mode1 = {{211, 1}, {-211, 1}, {111, 1}};
static const map<PdgId, unsigned int>& mode2 = {{111, 3}};
DecayedParticles ETA = apply<DecayedParticles>(event, "ETA");
// loop over particles
for (unsigned int ix = 0; ix < ETA.decaying().size(); ++ix) {
// select right decay mode
if (ETA.decaying()[ix].pid() == PID::ETA && ETA.modeMatches(ix, 3, mode1)) {
const Particle& pi0 = ETA.decayProducts()[ix].at(111)[0];
const Particle& pip = ETA.decayProducts()[ix].at(211)[0];
const Particle& pim = ETA.decayProducts()[ix].at(-211)[0];
double s1 = (pi0.momentum() + pim.momentum()).mass2();
double s2 = (pi0.momentum() + pip.momentum()).mass2();
double s3 = (pip.momentum() + pim.momentum()).mass2();
double mOut = pi0.mass() + pip.mass() + pim.mass();
double Q = ETA.decaying()[ix].mass() - mOut;
double X = sqrt(3.) / 2. / ETA.decaying()[ix].mass() / Q * (s1 - s2);
double Y = 3. * (sqr(ETA.decaying()[ix].mass() - pi0.mass()) - s3) / 2. / ETA.decaying()[ix].mass()
/ Q
- 1.;
_h[0]->fill(X);
_h[1]->fill(Y);
}
else if (ETA.modeMatches(ix, 3, mode2)) {
const Particles& pi0 = ETA.decayProducts()[ix].at(111);
double s1 = (pi0[2].momentum() + pi0[1].momentum()).mass2();
double s2 = (pi0[2].momentum() + pi0[0].momentum()).mass2();
double s3 = (pi0[0].momentum() + pi0[1].momentum()).mass2();
double mOut = pi0[2].mass() + pi0[0].mass() + pi0[1].mass();
double Q = ETA.decaying()[ix].mass() - mOut;
double X = sqrt(3.) / 2. / ETA.decaying()[ix].mass() / Q * (s1 - s2);
double Y = 3. * (sqr(ETA.decaying()[ix].mass() - pi0[2].mass()) - s3) / 2.
/ ETA.decaying()[ix].mass() / Q
- 1.;
double Z = sqr(X) + sqr(Y);
if (ETA.decaying()[ix].pid() == PID::ETA)
_h[2]->fill(Z);
else
_h[3]->fill(Z);
}
}
}
/// Normalise histograms etc., after the run
void finalize() {
for (unsigned int ix = 0; ix < 4; ++ix) normalize(_h[ix]);
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h[4];
/// @}
};
RIVET_DECLARE_PLUGIN(BESIII_2015_I1376484);
}