Rivet analyses
Exclusive D0 → K−ℓ+νℓ and D+ → K̄0ℓ+νℓ decays
Experiment: BESIII (BEPC)
Inspire ID: 2819140
Status: VALIDATED NOHEPDATA
Authors: - Peter Richardson
References: - arXiv: 2408.09087
Beams: * *
Beam energies: ANY
Run details: - Events with D-decays, either particle guns or collisions.
Differential decay rates for semi-leptonic D0 → K−ℓ+νℓ and D+ → K̄0ℓ+νℓ decays
Source
code:BESIII_2024_I2819140.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief D0 -> K- ell+ nu_ell and D+ -> Kbar0 ell+ nu_ell
class BESIII_2024_I2819140 : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(BESIII_2024_I2819140);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// Initialise and register projections
declare(UnstableParticles(Cuts::abspid==411 || Cuts::abspid==421 ), "UFS");
for(unsigned int ix=0;ix<4;++ix) {
book(_h[ix], 1+ix , 1 ,1);
if(ix>1) continue;
book(_c[ix], "TMP/c_"+toString(ix+1));
}
}
// Calculate the Q2 using mother and daugher meson
double q2(const Particle& B, int mesonID) {
FourMomentum q = B.mom() - select(B.children(), Cuts::pid==mesonID)[0];
return q*q;
}
// Check for explicit decay into pdgids
bool isSemileptonicDecay(const Particle& mother, vector<int> ids) {
// Trivial check to ignore any other decays but the one in question modulo photons
const Particles children = mother.children(Cuts::pid!=PID::PHOTON);
if (children.size()!=ids.size()) return false;
// Check for the explicit decay
return all(ids, [&](int i){return count(children, hasPID(i))==1;});
}
/// Perform the per-event analysis
void analyze(const Event& event) {
// Loop over D mesons
for (const Particle& p : apply<UnstableParticles>(event, "UFS").particles()) {
if(p.pid()==421) {
_c[0]->fill();
if(isSemileptonicDecay(p, {PID::KMINUS, PID::EPLUS, PID::NU_E})) {
_h[0]->fill(q2(p, PID::KMINUS));
}
else if(isSemileptonicDecay(p, {PID::KMINUS, PID::ANTIMUON, PID::NU_MU})) {
_h[1]->fill(q2(p, PID::KMINUS));
}
}
else if(p.pid()==-421) {
_c[0]->fill();
if(isSemileptonicDecay(p, {PID::KPLUS, PID::EMINUS, PID::NU_EBAR})) {
_h[0]->fill(q2(p, PID::KPLUS));
}
else if(isSemileptonicDecay(p, {PID::KPLUS, PID::MUON, PID::NU_MUBAR})) {
_h[1]->fill(q2(p, PID::KPLUS));
}
}
else if(p.pid()==411) {
_c[1]->fill();
if(isSemileptonicDecay(p, {-311, PID::EPLUS, PID::NU_E})) {
_h[2]->fill(q2(p, -311));
}
else if(isSemileptonicDecay(p, {-311, PID::ANTIMUON, PID::NU_MU})) {
_h[3]->fill(q2(p, -311));
}
else if(isSemileptonicDecay(p, { 130, PID::EPLUS, PID::NU_E})) {
_h[2]->fill(q2(p, 130));
}
else if(isSemileptonicDecay(p, { 130, PID::ANTIMUON, PID::NU_MU})) {
_h[3]->fill(q2(p, 130));
}
else if(isSemileptonicDecay(p, { 310, PID::EPLUS, PID::NU_E})) {
_h[2]->fill(q2(p, 310));
}
else if(isSemileptonicDecay(p, { 310, PID::ANTIMUON, PID::NU_MU})) {
_h[3]->fill(q2(p, 310));
}
}
else if(p.pid()==-411) {
_c[1]->fill();
if(isSemileptonicDecay(p, {311, PID::EMINUS, PID::NU_EBAR})) {
_h[2]->fill(q2(p, 311));
}
else if(isSemileptonicDecay(p, {311, PID::MUON, PID::NU_MUBAR})) {
_h[3]->fill(q2(p, 311));
}
else if(isSemileptonicDecay(p, { 130, PID::EMINUS, PID::NU_EBAR})) {
_h[2]->fill(q2(p, 130));
}
else if(isSemileptonicDecay(p, { 130, PID::MUON, PID::NU_MUBAR})) {
_h[3]->fill(q2(p, 130));
}
else if(isSemileptonicDecay(p, { 310, PID::EMINUS, PID::NU_EBAR})) {
_h[2]->fill(q2(p, 310));
}
else if(isSemileptonicDecay(p, { 310, PID::MUON, PID::NU_MUBAR})) {
_h[3]->fill(q2(p, 310));
}
}
}
}
/// Normalise histograms etc., after the run
void finalize() {
// lifetimes from PDG 2022 [ns] (as in paper)
double tau[2] = {410.3e-6, 1033e-6};
for(unsigned int ix=0;ix<4;++ix)
scale(_h[ix],1./tau[ix/2]/ *_c[ix/2]);
}
/// @}
/// @name Histograms
/// @{
Histo1DPtr _h[4];
CounterPtr _c[2];
/// @}
};
RIVET_DECLARE_PLUGIN(BESIII_2024_I2819140);
}