Rivet analyses
Helicity angle distributions in excited Ds meson decays
Experiment: BABAR (PEP-II)
Inspire ID: 827985
Status: VALIDATED
Authors: - Peter Richardson
References: - Phys.Rev.D 80 (2009) 092003
Beams: * *
Beam energies: ANY
Run details: - Any process producing excited Ds mesons
The decays Ds** → D*+KS0 → D0π+KS0 are used to measure the helicity angle, i.e. the angle between the pion and kaon in the rest frame of the D*. The decays of Ds1*(2700)+ and with mass 2.8 GeV were measured. It is unclear if this is the Ds1*(2860)+, Ds3*(2860)+ or a mixture of the two. This histogram is therefore filled we with each state and the admixture. The data were read from the plots in the papers.
Source
code:BABAR_2009_I827985.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief D**_s decays
class BABAR_2009_I827985 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(BABAR_2009_I827985);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// Initialise and register projections
declare(UnstableParticles(), "UFS");
// Book histograms
book(_h_DStar_ctheta, 1,1,1);
book(_h_D3_ctheta[0], 1,1,2);
book(_h_D3_ctheta[1], 1,1,3);
book(_h_D3_ctheta[2], 1,1,4);
}
/// Recursively walk the decay tree to find decay products of @a p
void findDecayProducts(Particle mother, Particles & dstar, Particles & d0, Particles & K0, Particles & pi, unsigned int & ncount) {
for(const Particle & p: mother.children()) {
if(p.abspid()==413)
dstar.push_back(p);
else if(p.abspid()==421)
d0.push_back(p);
else if(p.abspid()==130 || p.abspid()==130 || p.abspid()==311)
K0.push_back(p);
else if(p.abspid()==211)
pi.push_back(p);
ncount +=1;
}
}
/// Perform the per-event analysis
void analyze(const Event& event) {
for(const Particle& p : apply<UnstableParticles>(event, "UFS").particles(Cuts::abspid==100433 || Cuts::abspid==437 ||
Cuts::abspid==30433)) {
// decay products
Particles dstar,d0,K0,pi;
unsigned int ncount=0;
findDecayProducts(p, dstar, d0, K0, pi, ncount);
if(ncount!=2 || dstar.size()!=1 || K0.size()!=1 ) continue;
if(dstar[0].pid()/p.pid()<0) continue;
Particle p2 = dstar[0];
LorentzTransform boost = LorentzTransform::mkFrameTransformFromBeta(p2.momentum().betaVec());
Vector3 d1 = boost.transform(K0[0].momentum()).p3().unit();
ncount=0;
dstar.clear();
d0.clear();
pi.clear();
findDecayProducts(p2, dstar, d0, K0, pi, ncount);
if(ncount!=2 || pi.size()!=1 || d0.size()!=1 ) continue;
if(pi[0].pid()/p2.pid()<0) continue;
Vector3 d2 = boost.transform(pi[0].momentum()).p3().unit();
double cTheta = d1.dot(d2);
// decay angles
if(p.abspid()==100433)
_h_DStar_ctheta->fill(cTheta);
else if(p.abspid()==30433) {
_h_D3_ctheta[0]->fill(cTheta);
_h_D3_ctheta[2]->fill(cTheta);
}
else if(p.abspid()==437) {
_h_D3_ctheta[1]->fill(cTheta);
_h_D3_ctheta[2]->fill(cTheta);
}
}
}
/// Normalise histograms etc., after the run
void finalize() {
normalize(_h_DStar_ctheta);
normalize(_h_D3_ctheta[0]);
normalize(_h_D3_ctheta[1]);
normalize(_h_D3_ctheta[2]);
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h_DStar_ctheta,_h_D3_ctheta[3];
/// @}
};
RIVET_DECLARE_PLUGIN(BABAR_2009_I827985);
}