Rivet analyses
Mass distributions in τ decays with KS0 mesons
Experiment: CLEOII (CESR)
Inspire ID: 415408
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - Phys.Rev.D 53 (1996) 6037-6053
Beams: * *
Beam energies: ANY
Run details: - Any process producing tau leptons, originally e+e-
Mass distributions in the decays τ → ντ + KS0π−, K−KS0, KS0π−π0, KS0K−π0 and KS0KS0π−. The background subtracted data were read from the figures in the paper.
Source
code:CLEOII_1996_I415408.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/DecayedParticles.hh"
#include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief tau -> hadrons with KS0
class CLEOII_1996_I415408 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(CLEOII_1996_I415408);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// Initialise and register projections
UnstableParticles ufs = UnstableParticles(Cuts::abspid == 15);
declare(ufs, "UFS");
DecayedParticles TAU(ufs);
TAU.addStable(310);
TAU.addStable(111);
declare(TAU, "TAU");
// histos
for (unsigned int ix = 0; ix < 4; ++ix) {
book(_h[ix], 1 + ix, 1, 1);
if (ix > 1) continue;
book(_h[4 + ix], 5, 1, 1 + ix);
book(_h[6 + ix], 6 + ix, 1, 1);
}
}
/// Perform the per-event analysis
void analyze(const Event& event) {
DecayedParticles TAU = apply<DecayedParticles>(event, "TAU");
// loop over particles
for (unsigned int ix = 0; ix < TAU.decaying().size(); ++ix) {
int sign = TAU.decaying()[ix].pid() > 0 ? 1 : -1;
if ((TAU.modeMatches(ix, 3, mode1) || TAU.modeMatches(ix, 3, mode1CC))) {
const Particle& pim = TAU.decayProducts()[ix].at(-211 * sign)[0];
const Particle& K0 = TAU.decayProducts()[ix].at(310)[0];
_h[0]->fill((pim.mom() + K0.mom()).mass());
}
else if (TAU.modeMatches(ix, 3, mode2) || TAU.modeMatches(ix, 3, mode2CC)) {
const Particle& Km = TAU.decayProducts()[ix].at(-321 * sign)[0];
const Particle& K0 = TAU.decayProducts()[ix].at(310)[0];
_h[1]->fill((Km.mom() + K0.mom()).mass());
}
else if (TAU.modeMatches(ix, 4, mode3) || TAU.modeMatches(ix, 4, mode3CC)) {
const Particle& pim = TAU.decayProducts()[ix].at(-211 * sign)[0];
const Particle& K0 = TAU.decayProducts()[ix].at(310)[0];
const Particle& pi0 = TAU.decayProducts()[ix].at(111)[0];
_h[2]->fill((pim.mom() + K0.mom() + pi0.mom()).mass());
}
else if (TAU.modeMatches(ix, 4, mode4) || TAU.modeMatches(ix, 4, mode4CC)) {
const Particle& Km = TAU.decayProducts()[ix].at(-321 * sign)[0];
const Particle& K0 = TAU.decayProducts()[ix].at(310)[0];
const Particle& pi0 = TAU.decayProducts()[ix].at(111)[0];
_h[3]->fill((Km.mom() + K0.mom() + pi0.mom()).mass());
_h[4]->fill((Km.mom() + pi0.mom()).mass());
_h[5]->fill((K0.mom() + pi0.mom()).mass());
}
else if (TAU.modeMatches(ix, 4, mode5) || TAU.modeMatches(ix, 4, mode5CC)) {
const Particle& pim = TAU.decayProducts()[ix].at(-211 * sign)[0];
const Particles& K0 = TAU.decayProducts()[ix].at(310);
_h[6]->fill((pim.mom() + K0[0].mom() + K0[1].mom()).mass());
_h[7]->fill((pim.mom() + K0[0].mom()).mass());
_h[7]->fill((pim.mom() + K0[1].mom()).mass());
}
}
}
/// Normalise histograms etc., after the run
void finalize() {
normalize(_h, 1.0, false);
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h[8];
const map<PdgId, unsigned int> mode1 = {{310, 1}, {-211, 1}, {16, 1}};
const map<PdgId, unsigned int> mode1CC = {{310, 1}, {211, 1}, {-16, 1}};
const map<PdgId, unsigned int> mode2 = {{310, 1}, {-321, 1}, {16, 1}};
const map<PdgId, unsigned int> mode2CC = {{310, 1}, {321, 1}, {-16, 1}};
const map<PdgId, unsigned int> mode3 = {{310, 1}, {-211, 1}, {111, 1}, {16, 1}};
const map<PdgId, unsigned int> mode3CC = {{310, 1}, {211, 1}, {111, 1}, {-16, 1}};
const map<PdgId, unsigned int> mode4 = {{310, 1}, {-321, 1}, {111, 1}, {16, 1}};
const map<PdgId, unsigned int> mode4CC = {{310, 1}, {321, 1}, {111, 1}, {-16, 1}};
const map<PdgId, unsigned int> mode5 = {{310, 2}, {-211, 1}, {16, 1}};
const map<PdgId, unsigned int> mode5CC = {{310, 2}, {211, 1}, {-16, 1}};
/// @}
};
RIVET_DECLARE_PLUGIN(CLEOII_1996_I415408);
}