Rivet analyses
Mass distributions in B0 → KS0π+π− decays
Experiment: BABAR (PEP-II)
Inspire ID: 821188
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - Phys.Rev.D 80 (2009) 112001
Beams: * *
Beam energies: ANY
Run details: - Any process producing B0, originally Upsilon(4S) decay
Measurement of mass distributions in B0 → KS0π+π− decays. The data were read from the plots in the paper and may not be corrected for efficiency/acceptance, however the backgrounds shown in the paper have been subtracted.
Source
code:BABAR_2009_I821188.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/DecayedParticles.hh"
#include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief B0 > KS0 pi+ pi-
class BABAR_2009_I821188 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(BABAR_2009_I821188);
/// @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(PID::K0S);
declare(B0, "B0");
// histograms
for (unsigned int ix = 0; ix < 2; ++ix)
for (unsigned int iy = 0; iy < 2; ++iy) book(_h[ix][iy], 1 + ix, 1, 1 + iy);
}
/// Perform the per-event analysis
void analyze(const Event& event) {
static const map<PdgId, unsigned int>& mode = {{310, 1}, {211, 1}, {-211, 1}};
DecayedParticles B0 = apply<DecayedParticles>(event, "B0");
// loop over particles
for (unsigned int ix = 0; ix < B0.decaying().size(); ++ix) {
if (!B0.modeMatches(ix, 3, mode)) continue;
int sign = B0.decaying()[ix].pid() > 0 ? 1 : -1;
// boost to B rest frame
LorentzTransform boost = LorentzTransform::mkFrameTransformFromBeta(
B0.decaying()[ix].momentum().betaVec());
// momenta
FourMomentum pip = boost.transform(B0.decayProducts()[ix].at(211 * sign)[0].momentum());
FourMomentum pim = boost.transform(B0.decayProducts()[ix].at(-211 * sign)[0].momentum());
FourMomentum K0 = boost.transform(B0.decayProducts()[ix].at(310)[0].momentum());
// pi+pi- resonance
FourMomentum ppipi = pim + pip;
LorentzTransform boost2 = LorentzTransform::mkFrameTransformFromBeta(ppipi.betaVec());
double cTheta = boost2.transform(pim).p3().unit().dot(K0.p3().unit());
if (cTheta > 0.)
_h[0][0]->fill(ppipi.mass());
else
_h[0][1]->fill(ppipi.mass());
// K pi- resonance
FourMomentum pKpim = K0 + pim;
boost2 = LorentzTransform::mkFrameTransformFromBeta(pKpim.betaVec());
cTheta = boost2.transform(K0).p3().unit().dot(pip.p3().unit());
if (cTheta > 0.)
_h[1][0]->fill(pKpim.mass());
else
_h[1][1]->fill(pKpim.mass());
// K pi+ resonance
FourMomentum pKpip = K0 + pip;
boost2 = LorentzTransform::mkFrameTransformFromBeta(pKpip.betaVec());
cTheta = boost2.transform(pip).p3().unit().dot(pim.p3().unit());
if (cTheta > 0.)
_h[1][0]->fill(pKpip.mass());
else
_h[1][1]->fill(pKpip.mass());
}
}
/// Normalise histograms etc., after the run
void finalize() {
for (unsigned int ix = 0; ix < 2; ++ix)
for (unsigned int iy = 0; iy < 2; ++iy) normalize(_h[ix][iy], 1., false);
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h[2][2];
/// @}
};
RIVET_DECLARE_PLUGIN(BABAR_2009_I821188);
}