Rivet analyses
Spectral functions in τ− → π−π−π+π0ντ
Experiment: CLEOII (CESR)
Inspire ID: 505170
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - Phys.Rev.D 61 (2000) 072003
Beams: * *
Beam energies: ANY
Run details: - Any process producing tau leptons, originally e+e-
Measurement of the spectral functions for τ− → π−π−π+π0ντ, τ− → π−ωντ and non-ω τ− → π−π−π+π0ντ. The helicity angle in τ− → π−ωντ and mass distributions are also measured.
Source
code:CLEOII_2000_I505170.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/UnstableParticles.hh"
#include "Rivet/Projections/DecayedParticles.hh"
namespace Rivet {
/// @brief tau -> 4 pions
class CLEOII_2000_I505170 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(CLEOII_2000_I505170);
/// @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);
TAU.addStable(221);
declare(TAU, "TAU");
// histos
for (unsigned int ix=0; ix<6; ++ix) {
book(_h_mass[ix], 3, 1, 1+ix);
if (ix>2) continue;
book(_h_spect[ix], 1, 1, 1+ix);
}
book(_h_angle, 2, 1, 1);
book(_c,"TMP/nTau");
}
/// 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) {
_c->fill();
int sign = TAU.decaying()[ix].pid()>0 ? 1 : -1;
if (!(TAU.modeMatches(ix,5,mode ) ||
TAU.modeMatches(ix,5,modeCC))) continue;
const Particle & pi0 = TAU.decayProducts()[ix].at( 111 )[0];
const Particles & pim = TAU.decayProducts()[ix].at(-211*sign);
const Particle & pip = TAU.decayProducts()[ix].at( 211*sign)[0];
FourMomentum phad = pim[0].mom()+pim[1].mom()+pip.mom()+pi0.mom();
const double q = phad.mass();
const double mtau = TAU.decaying()[ix].mass();
_h_spect[0]->fill(phad.mass(),sqr(mtau)*mtau/q/sqr(sqr(mtau)-sqr(q))/(sqr(mtau)+2.*sqr(q)));
Particle omega;
int iomega=-1;
for (unsigned int ix=0; ix<2; ++ix) {
Particle parent = pim[ix];
while (!parent.parents().empty()) {
parent = parent.parents()[0];
if (parent.pid()==223) break;
}
if (parent.pid()==223) {
omega=parent;
iomega=ix;
}
}
if (iomega>=0) {
_h_spect[1]->fill(phad.mass(),sqr(mtau)*mtau/q/sqr(sqr(mtau)-sqr(q))/(sqr(mtau)+2.*sqr(q)));
const int ibatch = iomega == 0 ? 1 : 0;
const LorentzTransform boost = LorentzTransform::mkFrameTransformFromBeta(omega.mom().betaVec());
const Vector3 axis = boost.transform(pim[ibatch].mom());
const FourMomentum ppi0 = boost.transform(pi0.mom());
const FourMomentum ppip = boost.transform(pip.mom());
const Vector3 norm = ppi0.p3().cross(pip.p3()).unit();
const double cTheta = axis.dot(norm);
_h_angle->fill(cTheta);
}
else {
_h_spect[2]->fill(phad.mass(),sqr(mtau)*mtau/q/sqr(sqr(mtau)-sqr(q))/(sqr(mtau)+2.*sqr(q)));
}
_h_mass[0]->fill((phad-pim[0].mom()).mass());
_h_mass[0]->fill((phad-pim[1].mom()).mass());
_h_mass[1]->fill((pim[0].mom()+pi0.mom()).mass());
_h_mass[1]->fill((pim[1].mom()+pi0.mom()).mass());
_h_mass[2]->fill((pim[1].mom()+pip.mom()).mass());
_h_mass[3]->fill((pip .mom()+pi0.mom()).mass());
_h_mass[4]->fill(q);
_h_mass[5]->fill((phad-pi0.mom()).mass());
}
}
/// Normalise histograms etc., after the run
void finalize() {
const double Gamma = 6.582119514e-25/290.3e-15;
const double GF = 1.1663787e-5;
const double cosC = 0.97373;
scale(_h_spect, Gamma*16.*sqr(M_PI)/sqr(GF*cosC)/ *_c);
normalize(_h_mass, 1.0, false);
normalize(_h_angle, 1.0, false);
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h_spect[3],_h_angle,_h_mass[6];
CounterPtr _c;
const map<PdgId,unsigned int> mode = { { 111,1},{-211,2},{ 211,1},{ 16,1}};
const map<PdgId,unsigned int> modeCC = { { 111,1},{ 211,2},{-211,1},{-16,1}};
/// @}
};
RIVET_DECLARE_PLUGIN(CLEOII_2000_I505170);
}