Rivet analyses
Helicity angle distributions in excited Ds meson decays
Experiment: LHCB (LHC)
Inspire ID: 1414195
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - JHEP 02 (2016) 133
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(2536)+, Ds2*(2573)+, Ds1*(2700)+, DsJ*(2860)+, DsJ(3040)+ were measured, currently the DsJ(3040)+ is not implemented. It is unclear if the DsJ*(2860)+ 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 extracted from the files supplied on the LHCb website.
Source
code:LHCB_2016_I1414195.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief D**_s decays
class LHCB_2016_I1414195 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(LHCB_2016_I1414195);
/// @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_DStar_ctheta, 2, 1, 1);
book(_h_D3_ctheta[0], 2, 1, 2);
book(_h_D3_ctheta[1], 2, 1, 4);
book(_h_D3_ctheta[2], 2, 1, 5);
}
/// 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 == 435 || Cuts::abspid == 10433 || 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() == 435)
_h_D2_ctheta->fill(cTheta);
else if (p.abspid() == 10433)
_h_D1_ctheta->fill(cTheta);
else 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_D1_ctheta);
normalize(_h_D2_ctheta);
normalize(_h_DStar_ctheta);
normalize(_h_D3_ctheta[0]);
normalize(_h_D3_ctheta[1]);
normalize(_h_D3_ctheta[2]);
}
///@}
/// @name Histograms
///@{
Histo1DPtr _h_D1_ctheta, _h_D2_ctheta, _h_DStar_ctheta, _h_D3_ctheta[3];
///@}
};
RIVET_DECLARE_PLUGIN(LHCB_2016_I1414195);
}