Rivet analyses
3π mass distribution in τ− → π−π−π+ντ decays
Experiment: ARGUS (DORIS)
Inspire ID: 339268
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - Z.Phys.C 58 (1993) 61-70
Beams: * *
Beam energies: ANY
Run details: - Any process producing tau leptons, originally e+e- > tau+tau-
Three pion mass distrubution in τ− → π−π−π+ντ decays. Data take from the tables in the paper.
Source
code:ARGUS_1992_I339268.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/DecayedParticles.hh"
#include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief tau -> 3 pi
class ARGUS_1992_I339268 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(ARGUS_1992_I339268);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// Initialise and register projections
UnstableParticles ufs(Cuts::abspid == 15);
declare(ufs, "UFS");
DecayedParticles TAU(ufs);
TAU.addStable(310);
TAU.addStable(111);
declare(TAU, "TAU");
// histos
book(_h_mass, 1, 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, 4, mode) || TAU.modeMatches(ix, 4, modeCC))) {
continue;
}
const Particles& pip = TAU.decayProducts()[ix].at(211 * sign);
const Particles& pim = TAU.decayProducts()[ix].at(-211 * sign);
double Q2 = (pip[0].mom() + pim[0].mom() + pim[1].mom()).mass2();
_h_mass->fill(sqrt(Q2));
}
}
/// Normalise histograms etc., after the run
void finalize() {
normalize(_h_mass, 1., false);
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h_mass;
const map<PdgId, unsigned int> mode = {{-211, 2}, {211, 1}, {16, 1}};
const map<PdgId, unsigned int> modeCC = {{211, 2}, {-211, 1}, {-16, 1}};
/// @}
};
RIVET_DECLARE_PLUGIN(ARGUS_1992_I339268);
}