Rivet analyses
Helicity angle distributions in excited D meson decays
Experiment: BABAR (PEP-II)
Inspire ID: 867611
Status: VALIDATED
Authors: - Peter Richardson
References: - Phys.Rev. D82 (2010) 111101
Beams: * *
Beam energies: ANY
Run details: - Any process producing excited D mesons
The decays D** → D*+π− → D0π+π− are used to measure the helicity angle, i.e. the angle between the two pions in the rest frame of the D*. The decays of D1(2420)0, D2*(2460)0, D(2550)0, D*(2600), D(2750) were measured. The data were read from the plots in the papers and therefore for the D1(2420)0, D2*(2460)0 the error bars are the size of the points in the plots.
Source
code:BABAR_2010_I867611.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief D_1 and D_2 decay distributions
class BABAR_2010_I867611 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(BABAR_2010_I867611);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// Initialise and register projections
declare(UnstableParticles(), "UFS");
// Book histograms
book(_h_D1_ctheta, 1, 1, 1);
book(_h_D2_ctheta, 1, 1, 2);
book(_h_D02S_ctheta, 1, 1, 3);
book(_h_DStar02S_ctheta, 1, 1, 4);
book(_h_D3_ctheta, 1, 1, 5);
}
/// Recursively walk the decay tree to find decay products of @a p
void findDecayProducts(Particle mother,
Particles& dstar,
Particles& d0,
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() == 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 == 425 || Cuts::abspid == 10423 || Cuts::abspid == 100421
|| Cuts::abspid == 100423 || Cuts::abspid == 427)) {
// decay products
Particles dstar, d0, pi;
unsigned int ncount = 0;
findDecayProducts(p, dstar, d0, pi, ncount);
if (ncount != 2 || dstar.size() != 1 || pi.size() != 1 || d0.size() != 0) continue;
if (dstar[0].pid() / p.pid() < 0) continue;
Particle p2 = dstar[0];
LorentzTransform boost = LorentzTransform::mkFrameTransformFromBeta(p2.momentum().betaVec());
Vector3 d1 = boost.transform(pi[0].momentum()).p3().unit();
ncount = 0;
dstar.clear();
d0.clear();
pi.clear();
findDecayProducts(p2, dstar, d0, pi, ncount);
if (ncount != 2 || dstar.size() != 0 || 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() == 425)
_h_D2_ctheta->fill(cTheta);
else if (p.abspid() == 10423)
_h_D1_ctheta->fill(cTheta);
else if (p.abspid() == 100421)
_h_D02S_ctheta->fill(cTheta);
else if (p.abspid() == 100423)
_h_DStar02S_ctheta->fill(cTheta);
else if (p.abspid() == 427)
_h_D3_ctheta->fill(cTheta);
}
}
/// Normalise histograms etc., after the run
void finalize() {
normalize(_h_D1_ctheta);
normalize(_h_D2_ctheta);
normalize(_h_D02S_ctheta);
normalize(_h_DStar02S_ctheta);
normalize(_h_D3_ctheta);
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h_D1_ctheta, _h_D2_ctheta, _h_D02S_ctheta;
Histo1DPtr _h_DStar02S_ctheta, _h_D3_ctheta;
/// @}
};
RIVET_DECLARE_PLUGIN(BABAR_2010_I867611);
}