Rivet analyses
Mass and angular distributions in B0 → ϕKπ
Experiment: BABAR (PEP-II)
Inspire ID: 792439
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - Phys.Rev.D 78 (2008) 092008
Beams: * *
Beam energies: ANY
Run details: - Any process producing B0, originally Upsilon(4S) decay
Measurment of mass and angular distributions in B0 → ϕKπ decays. The corrected data were read from the figures in the paper.
Source
code:BABAR_2008_I792439.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/UnstableParticles.hh"
#include "Rivet/Projections/DecayedParticles.hh"
namespace Rivet {
/// @brief B -> phi K pi
class BABAR_2008_I792439 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(BABAR_2008_I792439);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// Initialise and register projections
UnstableParticles ufs = UnstableParticles(Cuts::abspid==511);
declare(ufs, "UFS");
DecayedParticles B0(ufs);
B0.addStable(333);
B0.addStable(310);
B0.addStable(111);
declare(B0, "B0");
// histos
for(unsigned int ix=0;ix<2;++ix) {
book(_p[ix][0],1,2,2+ix);
book(_p[ix][1],"TMP/norm_"+toString(ix));
for(unsigned int iy=0;iy<2;++iy) {
book(_h_mass[ix][iy],2,1+ix,1+iy);
book(_h_angle[ix][iy],3+ix,1,1+iy);
}
}
}
/// Perform the per-event analysis
void analyze(const Event& event) {
static const map<PdgId,unsigned int> & mode1 = { { 321,1},{-211,1}, { 333,1}};
static const map<PdgId,unsigned int> & mode1CC = { {-321,1},{ 211,1}, { 333,1}};
static const map<PdgId,unsigned int> & mode2 = { { 310,1},{ 111,1}, { 333,1}};
DecayedParticles B0 = apply<DecayedParticles>(event, "B0");
// loop over particles
for(unsigned int ix=0;ix<B0.decaying().size();++ix) {
int sign = 1,imode=-1;
if (B0.modeMatches(ix,3,mode1)) {
imode = 0;
sign = 1;
}
else if(B0.modeMatches(ix,3,mode1CC)) {
imode = 0;
sign =-1;
}
else if(B0.modeMatches(ix,3,mode2)) {
imode = 1;
sign = 1;
}
else
continue;
// particles
const Particle & KK = B0.decayProducts()[ix].at(imode==0 ? 321*sign : 310)[0];
const Particle & pi = B0.decayProducts()[ix].at(imode==0 ? -211*sign : 111)[0];
const Particle & phi = B0.decayProducts()[ix].at( 333 )[0];
// children of the phi
if(phi.children().size()!=2) continue;
if(phi.children()[0].abspid()!=321) continue;
if(phi.children()[0].pid()!=-phi.children()[1].pid()) continue;
double mKpi = (KK.momentum()+pi.momentum()).mass();
_h_mass[imode][0]->fill(mKpi);
_h_mass[imode][1]->fill(phi.mass());
Particle Kp1 = phi.children()[0];
Particle Km1 = phi.children()[1];
// B0 frame
LorentzTransform boost1 = LorentzTransform::mkFrameTransformFromBeta(B0.decaying()[ix].momentum().betaVec());
FourMomentum pKstar = boost1.transform(KK.momentum()+pi.momentum());
FourMomentum pPhi = boost1.transform(phi.momentum());
// K pi helicity angle
LorentzTransform boost2 = LorentzTransform::mkFrameTransformFromBeta(pKstar.betaVec());
FourMomentum pKp = boost2.transform(boost1.transform(KK.momentum()));
Vector3 axis1 = pKstar.p3().unit();
double cTheta1 = axis1.dot(pKp.p3().unit());
// phi helicity angle
LorentzTransform boost3 = LorentzTransform::mkFrameTransformFromBeta(pPhi.betaVec());
FourMomentum pKp1 = boost3.transform(boost1.transform(Kp1.momentum()));
Vector3 axis2 = pPhi.p3().unit();
double cTheta2 = axis2.dot(pKp1.p3().unit());
if(mKpi>.75 && mKpi<1.05) {
_h_angle[0][0]->fill(cTheta1);
_h_angle[0][1]->fill(cTheta2);
_p[0][0]->fill(-0.5*(1-5.*sqr(cTheta2)));
_p[0][1]->fill();
}
else if(mKpi>1.13 && mKpi<1.53) {
_h_angle[1][0]->fill(cTheta1);
_h_angle[1][1]->fill(cTheta2);
_p[1][0]->fill(-0.5*(1-5.*sqr(cTheta2)));
_p[1][1]->fill();
}
}
}
/// Normalise histograms etc., after the run
void finalize() {
// histos
for(unsigned int ix=0;ix<2;++ix) {
scale(_p[ix][0], 1./ *_p[ix][1]);
for(unsigned int iy=0;iy<2;++iy) {
normalize(_h_mass[ix][iy] ,1.,false);
normalize(_h_angle[ix][iy],1.,false);
}
}
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h_mass[2][2],_h_angle[2][2];
CounterPtr _p[2][2];
/// @}
};
RIVET_DECLARE_PLUGIN(BABAR_2008_I792439);
}