Rivet analyses
ππ mass and helicity angle for B0 → ρ±π∓ and B+ → ρ0π+
Experiment: BELLE (KEKB)
Inspire ID: 589587
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - Phys.Lett.B 542 (2002) 183-192
Beams: * *
Beam energies: ANY
Run details: - Any process producing B mesons, originally Upsilon(4S) decays
Measurement of the ππ mass and helicity angle for B0 → ρ±π∓ and B+ → ρ0π+. The background subtracted data were read from figures 2 and 3 in the paper.
Source
code:BELLE_2002_I589587.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/UnstableParticles.hh"
#include "Rivet/Projections/DecayedParticles.hh"
namespace Rivet {
/// @brief B -> rho pi
class BELLE_2002_I589587 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(BELLE_2002_I589587);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// projections
UnstableParticles ufs = UnstableParticles(Cuts::abspid==511 || Cuts::abspid==521);
declare(ufs, "UFS");
DecayedParticles BB(ufs);
BB.addStable( 111);
declare(BB, "BB");
// histos
for (unsigned int ix=0; ix<2; ++ix) {
book(_h_mass [ix], 1, 1, 1+ix);
book(_h_angle[ix], 2, 1, 1+ix);
}
}
/// Perform the per-event analysis
void analyze(const Event& event) {
DecayedParticles BB = apply<DecayedParticles>(event, "BB");
for(unsigned int ix=0; ix<BB.decaying().size(); ++ix) {
int sign = BB.decaying()[ix].pid()/BB.decaying()[ix].abspid();
unsigned int imode=0;
if (BB.modeMatches(ix,3,mode1)) imode=0;
else if(sign== 1 && BB.modeMatches(ix,3,mode2 )) imode=1;
else if(sign==-1 && BB.modeMatches(ix,3,mode2CC)) imode=1;
else continue;
const Particles & pip = BB.decayProducts()[ix].at( sign*211);
const Particles & pim = BB.decayProducts()[ix].at(-sign*211);
bool pipiVeto=false;
Particle pRho[2];
double delta=1e30;
for (const Particle& p1 : pip) {
for(const Particle& p2 : pim) {
double mpipi = (p1.mom()+p2.mom()).mass();
if (abs(mpipi-1.86484)<0.14 ||
abs(mpipi-3.09690)<0.07 ||
abs(mpipi-3.68610)<0.05) {
pipiVeto=true;
break;
}
if (abs(mpipi-.77)<delta) {
delta= abs(mpipi-.77);
pRho[0]=p1;
pRho[1]=p2;
}
}
}
if (pipiVeto) continue;
if (imode==0) {
const Particle & pi0 = BB.decayProducts()[ix].at(111)[0];
delta=1e30;
for (const Particle& p1 : pip) {
double mpipi = (p1.mom()+pi0.mom()).mass();
if (abs(mpipi-1.86966)<0.05) {
pipiVeto=true;
break;
}
if (abs(mpipi-.77)<delta) {
delta= abs(mpipi-.77);
pRho[0]=p1;
pRho[1]=pi0;
}
}
if (pipiVeto) continue;
for (const Particle& p1 : pim) {
double mpipi = (p1.mom()+pi0.mom()).mass();
if (abs(mpipi-1.86966)<0.05) {
pipiVeto=true;
break;
}
if (abs(mpipi-.77)<delta) {
delta= abs(mpipi-.77);
pRho[0]=p1;
pRho[1]=pi0;
}
}
if (pipiVeto) continue;
}
FourMomentum prho = pRho[0].mom()+pRho[1].mom();
double mpipi = prho.mass();
_h_mass[imode]->fill(mpipi);
// check if we should compute helicty angle
if (imode==0 && (mpipi<.6 || mpipi>0.95)) continue;
else if (imode==1 && (mpipi<.62|| mpipi>0.92)) continue;
// compute the helicity angle
LorentzTransform boost1 = LorentzTransform::mkFrameTransformFromBeta(BB.decaying()[ix].mom().betaVec());
prho = boost1.transform(prho);
FourMomentum ppi = boost1.transform(pRho[0].mom());
LorentzTransform boost2 = LorentzTransform::mkFrameTransformFromBeta(prho.betaVec());
ppi = boost2.transform(ppi);
double cTheta = ppi.p3().unit().dot(prho.p3().unit());
_h_angle[imode]->fill(cTheta);
}
}
/// Normalise histograms etc., after the run
void finalize() {
normalize(_h_mass, 1.0, false);
normalize(_h_angle, 1.0, false);
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h_mass[2], _h_angle[2];
const map<PdgId,unsigned int> mode1 = { { 211,1}, {-211,1}, { 111,1} };
const map<PdgId,unsigned int> mode2 = { { 211,2}, {-211,1} };
const map<PdgId,unsigned int> mode2CC = { {-211,2}, { 211,1} };
/// @}
};
RIVET_DECLARE_PLUGIN(BELLE_2002_I589587);
}