Rivet analyses
Monte Carlo analysis to compute semi-leptonic branching ratios of heavy-flavour hadrons
Experiment: ()
Status: VALIDATED
Authors: - Ilia Kalaitzidou
References: none listed
Beams: * *
Beam energies: ANY
Run details: - Anything with heavy-flavour hadrons
Plots to study semi-leptonic decays of heavy-flavour hadrons (branching ratios, hadron and lepton pT.
Source
code:MC_HFBRANCHING.cc
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Math/LorentzTrans.hh"
#include "Rivet/Projections/FinalState.hh"
#include "Rivet/Projections/HeavyHadrons.hh"
namespace Rivet {
/// @brief MC analysis to compute semi-leptonic branching ratios of heavy-flavour hadrons
class MC_HFBRANCHING : public Analysis {
public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(MC_HFBRANCHING);
/// @name Analysis methods
/// @{
const string hadron_id(const int pid) const {
switch (pid) {
case PID::B0: return "B0";
case PID::BPLUS: return "BPLUS";
case PID::B0S: return "B0S";
case PID::LAMBDAB: return "LAMBDAB";
case PID::D0: return "D0";
case PID::DPLUS: return "DPLUS";
case PID::DSPLUS: return "DSPLUS";
case PID::LAMBDACPLUS: return "LAMBDACPLUS";
default: return "";
}
}
//Semi-leptonic decays with one hadron
const vector<int> decay_modes_3body(const int pid) const {
switch (pid) {
case PID::B0: return {413, 411, 10413, 10411, 20413, 415};
case PID::BPLUS: return {423, 421, 10423, 10421, 20423, 425};
case PID::B0S: return {433, 431, 10433, 10431, 20433, 435};
case PID::LAMBDAB: return {4122, 102142, 102144};
case PID::D0: return {323, 321, 10323, 325, 211, 213};
case PID::DPLUS: return {313, 311, 10313, 315, 111, 113, 221, 331, 231};
case PID::DSPLUS: return {333, 221, 331, 311, 313};
case PID::LAMBDACPLUS: return {3122, 3212, 3214, 2112, 2114};
default: return {};
}
}
//Semi-leptonic decays with two hadrons
const vector<int> decay_modes_4body(const int pid) const {
switch (pid) {
case PID::D0: return {321, 111, 211, 311};
case PID::DPLUS: return {311, 111, 321, 211};
case PID::DSPLUS: return {};
case PID::LAMBDACPLUS: return {211, 211, 111, 2112};
default: return {};
}
}
void fill_Histos(const string& hadron_type, const Particle& p) {
//********Find decay products of hadron*******//
vector<int> decay_par; //Vector with direct descendants in hadron decay
vector<double> child_pt_LAB, child_pt_COM; //Vector with pT of children from hadron decay
decay_par.clear(), decay_par.resize(0); //vector with hadron's direct descendants
child_pt_LAB.clear(), child_pt_LAB.resize(0); //vector with pT of hadron's direct descendants
child_pt_COM.clear(),
child_pt_COM.resize(0); //vector with pT of hadron's direct descendants in hadron's COM
for (const Particle& child : p.children()) {
decay_par.push_back(child.abspid()); //Get a list of the direct descendants from the current particle
child_pt_LAB.push_back(child.pT() / GeV);
// Reset the boost
_boost = combine(_boost, _boost.inverse());
_boost = LorentzTransform::mkFrameTransformFromBeta(p.momentum().betaVec());
Particle temp = p;
Particle temp_child = child;
// temp.setMomentum(_boost.transform(temp.momentum())); // to test that the boost works and gives hadron's pt=0
temp_child.setMomentum(
_boost.transform(temp_child.momentum())); //transform child's pt in hadron's COM
child_pt_COM.push_back(temp_child.pT() / GeV);
}
//remove photons from vector to consider QED radiation effects
decay_par.erase(std::remove(decay_par.begin(), decay_par.end(), 22), decay_par.end());
//********Compute branching fractions and fill histograms*******//
vector<int> Modes_3body = decay_modes_3body(p.abspid()); //vector with decay modes of 3-body decays
vector<int> Modes_4body = decay_modes_4body(p.abspid()); //some 4-body decays considered for c-hadrons
//Bins to be filled, different for b- and c-hadrons
int bin_position = -1;
int last_bin_position = -1;
bool found_decay_mode = false;
if (decay_par.size() == 3) { //Semileptonic decays with exactly three decay products
int lepton_position = -1; //Lepton position in decay_par vector
for (unsigned int i = 0; i < Modes_3body.size(); i++) {
if (contains(decay_par, Modes_3body[i])) {
_h["pt_" + hadron_id(p.abspid())]->fill(p.pT() / GeV); //hadron's pT
if (hadron_type == "b") {
bin_position = 3 * i; //For b-hadrons there are e, mu and tau decays
last_bin_position = 3 * Modes_3body.size() + 1;
}
else if (hadron_type == "c") {
bin_position = 2 * i; //For c-hadrons there are e and mu decays only
last_bin_position = 2 * Modes_3body.size() + Modes_4body.size() + 1;
}
else
cout << "I compute decays of heavy-flavour hadrons, pass b or c" << endl;
//electron decays
if ((contains(decay_par, 11) && contains(decay_par, 12))) {
_h[hadron_id(p.abspid()) + "_frac_clnu"]->fill(bin_position + 1); //branching fraction
//Place the e, mu and tau decays for each mode successively
found_decay_mode = true;
lepton_position = std::find(decay_par.begin(), decay_par.end(), 11) - decay_par.begin();
_h[hadron_id(p.abspid()) + "_e_pT"]->fill(child_pt_COM[lepton_position]); //lepton's pT
_h[hadron_id(p.abspid()) + "_lepton_pT_COM"]->fill(child_pt_COM[lepton_position]);
_h[hadron_id(p.abspid()) + "_lepton_pT_LAB"]->fill(child_pt_LAB[lepton_position]);
}
//muon decays
else if ((contains(decay_par, 13) && contains(decay_par, 14))) {
_h[hadron_id(p.abspid()) + "_frac_clnu"]->fill(bin_position + 2);
found_decay_mode = true;
lepton_position = std::find(decay_par.begin(), decay_par.end(), 13) - decay_par.begin();
_h[hadron_id(p.abspid()) + "_mu_pT"]->fill(child_pt_COM[lepton_position]);
_h[hadron_id(p.abspid()) + "_lepton_pT_COM"]->fill(child_pt_COM[lepton_position]);
_h[hadron_id(p.abspid()) + "_lepton_pT_LAB"]->fill(child_pt_LAB[lepton_position]);
}
//tau decays
else if ((contains(decay_par, 15) && contains(decay_par, 16))) {
_h[hadron_id(p.abspid()) + "_frac_clnu"]->fill(bin_position + 3);
found_decay_mode = true;
lepton_position = std::find(decay_par.begin(), decay_par.end(), 15) - decay_par.begin();
_h[hadron_id(p.abspid()) + "_tau_pT"]->fill(child_pt_COM[lepton_position]);
_h[hadron_id(p.abspid()) + "_lepton_pT_COM"]->fill(child_pt_COM[lepton_position]);
_h[hadron_id(p.abspid()) + "_lepton_pT_LAB"]->fill(child_pt_LAB[lepton_position]);
}
}
}
}
else if (decay_par.size() == 4
&& hadron_type == "c") { //Semileptonic decays with exactly four decay products
int lepton_position = -1;
for (unsigned int i = 0; i < Modes_4body.size(); i++) {
if (contains(decay_par, Modes_4body[i]) && contains(decay_par, Modes_4body[i + 1])) {
_h["pt_" + hadron_id(p.abspid())]->fill(p.pT() / GeV); //hadron's pT
bin_position = 2 * Modes_3body.size() + i; //place the 4-body decay modes after the 3-body ones
last_bin_position = 2 * Modes_3body.size() + Modes_4body.size() + 1;
//electron decays
if ((contains(decay_par, 11) && contains(decay_par, 12))) {
_h[hadron_id(p.abspid()) + "_frac_clnu"]->fill(bin_position + 1);
found_decay_mode = true;
lepton_position = std::find(decay_par.begin(), decay_par.end(), 11) - decay_par.begin();
_h[hadron_id(p.abspid()) + "_e_pT"]->fill(child_pt_COM[lepton_position]); //lepton's pT
_h[hadron_id(p.abspid()) + "_lepton_pT_COM"]->fill(child_pt_COM[lepton_position]);
_h[hadron_id(p.abspid()) + "_lepton_pT_LAB"]->fill(child_pt_LAB[lepton_position]);
}
//muon decays
else if ((contains(decay_par, 13) && contains(decay_par, 14))) {
_h[hadron_id(p.abspid()) + "_frac_clnu"]->fill(bin_position + 2);
found_decay_mode = true;
lepton_position = std::find(decay_par.begin(), decay_par.end(), 13) - decay_par.begin();
_h[hadron_id(p.abspid()) + "_mu_pT"]->fill(child_pt_COM[lepton_position]);
_h[hadron_id(p.abspid()) + "_lepton_pT_COM"]->fill(child_pt_COM[lepton_position]);
_h[hadron_id(p.abspid()) + "_lepton_pT_LAB"]->fill(child_pt_LAB[lepton_position]);
}
}
}
}
//Fill last bin of branching fractions with decays that don't fall into any category
if (!found_decay_mode) _h[hadron_id(p.abspid()) + "_frac_clnu"]->fill(last_bin_position);
}
/// Book histograms and initialise projections before the run
void init() {
declare(HeavyHadrons(Cuts::pT > 5. * GeV && Cuts::abseta < 2.5), "HA");
// histograms
//Branching ratios
//Include semi-leptonic decay modes only
book(_h["B0_frac_clnu"], "BR_B0_clnu", 19, 0.5, 19.5);
book(_h["B0S_frac_clnu"], "BR_B0S_clnu", 19, 0.5, 19.5);
book(_h["BPLUS_frac_clnu"], "BR_BPLUS_clnu", 19, 0.5, 19.5);
book(_h["LAMBDAB_frac_clnu"], "BR_LAMBDAB_clnu", 10, 0.5, 10.5);
book(_h["D0_frac_clnu"], "BR_D0_clnu", 17, 0.5, 17.5);
book(_h["DPLUS_frac_clnu"], "BR_DPLUS_clnu", 23, 0.5, 23.5);
book(_h["DSPLUS_frac_clnu"], "BR_DSPLUS_clnu", 11, 0.5, 11.5);
book(_h["LAMBDACPLUS_frac_clnu"], "BR_LAMBDACPLUS_clnu", 15, 0.5, 15.5);
//Hadron momentum
book(_h["pt_B0"], "B0_pT", 40, 0., 200.);
book(_h["pt_BPLUS"], "BPLUS_pT", 40, 0., 200.);
book(_h["pt_B0S"], "B0S_pT", 40, 0., 200.);
book(_h["pt_D0"], "D0_pT", 40, 0., 200.);
book(_h["pt_DPLUS"], "DPLUS_pT", 40, 0., 200.);
book(_h["pt_DSPLUS"], "DSPLUS_pT", 40, 0., 200.);
book(_h["pt_LAMBDAB"], "LAMBDAB_pT", 40, 0., 200.);
book(_h["pt_LAMBDACPLUS"], "LAMBDACPLUS_pT", 40, 0., 200.);
//Chared lepton momentum in LAB
book(_h["B0_lepton_pT_LAB"], "B0_lepton_pT_LAB", 20, 0., 100.);
book(_h["BPLUS_lepton_pT_LAB"], "BPLUS_lepton_pT_LAB", 20, 0., 100.);
book(_h["B0S_lepton_pT_LAB"], "B0S_lepton_pT_LAB", 20, 0., 100.);
book(_h["D0_lepton_pT_LAB"], "D0_lepton_pT_LAB", 20, 0., 100.);
book(_h["DPLUS_lepton_pT_LAB"], "DPLUS_lepton_pT_LAB", 20, 0., 100.);
book(_h["DSPLUS_lepton_pT_LAB"], "DSPLUS_lepton_pT_LAB", 20, 0., 100.);
book(_h["LAMBDAB_lepton_pT_LAB"], "LAMBDAB_lepton_pT_LAB", 20, 0., 100.);
book(_h["LAMBDACPLUS_lepton_pT_LAB"], "LAMBDACPLUS_lepton_pT_LAB", 20, 0., 100.);
//Chared lepton momentum in COM
book(_h["B0_e_pT"], "B0_e_pT", 25, 0., 2.5);
book(_h["B0_mu_pT"], "B0_mu_pT", 25, 0., 2.5);
book(_h["B0_tau_pT"], "B0_tau_pT", 25, 0., 2.5);
book(_h["B0_lepton_pT_COM"], "B0_lepton_pT_COM", 25, 0., 2.5);
book(_h["B0S_e_pT"], "B0S_e_pT", 25, 0., 2.5);
book(_h["B0S_mu_pT"], "B0S_mu_pT", 25, 0., 2.5);
book(_h["B0S_tau_pT"], "B0S_tau_pT", 25, 0., 2.5);
book(_h["B0S_lepton_pT_COM"], "B0S_lepton_pT_COM", 25, 0., 2.5);
book(_h["BPLUS_e_pT"], "BPLUS_e_pT", 25, 0., 2.5);
book(_h["BPLUS_mu_pT"], "BPLUS_mu_pT", 25, 0., 2.5);
book(_h["BPLUS_tau_pT"], "BPLUS_tau_pT", 25, 0., 2.5);
book(_h["BPLUS_lepton_pT_COM"], "BPLUS_lepton_pT_COM", 25, 0., 2.5);
book(_h["LAMBDAB_e_pT"], "LAMBDAB_e_pT", 25, 0., 2.5);
book(_h["LAMBDAB_mu_pT"], "LAMBDAB_mu_pT", 25, 0., 2.5);
book(_h["LAMBDAB_tau_pT"], "LAMBDAB_tau_pT", 25, 0., 2.5);
book(_h["LAMBDAB_lepton_pT_COM"], "LAMBDAB_lepton_pT_COM", 25, 0., 2.5);
book(_h["D0_e_pT"], "D0_e_pT", 15, 0., 1.5);
book(_h["D0_mu_pT"], "D0_mu_pT", 15, 0., 1.5);
book(_h["D0_lepton_pT_COM"], "D0_lepton_pT_COM", 15, 0., 1.5);
book(_h["DSPLUS_e_pT"], "DSPLUS_e_pT", 15, 0., 1.5);
book(_h["DSPLUS_mu_pT"], "DSPLUS_mu_pT", 15, 0., 1.5);
book(_h["DSPLUS_lepton_pT_COM"], "DSPLUS_lepton_pT_COM", 15, 0., 1.5);
book(_h["DPLUS_e_pT"], "DPLUS_e_pT", 15, 0., 1.5);
book(_h["DPLUS_mu_pT"], "DPLUS_mu_pT", 15, 0., 1.5);
book(_h["DPLUS_lepton_pT_COM"], "DPLUS_lepton_pT_COM", 15, 0., 1.5);
book(_h["LAMBDACPLUS_e_pT"], "LAMBDACPLUS_e_pT", 25, 0., 2.5);
book(_h["LAMBDACPLUS_mu_pT"], "LAMBDACPLUS_mu_pT", 25, 0., 2.5);
book(_h["LAMBDACPLUS_lepton_pT_COM"], "LAMBDACPLUS_lepton_pT_COM", 25, 0., 2.5);
}
/// Perform the per-event analysis
void analyze(const Event& event) {
const HeavyHadrons& ha = apply<HeavyHadrons>(event, "HA");
if (ha.bHadrons().empty() && ha.cHadrons().empty()) vetoEvent;
//b hadrons branching ratios
for (const Particle& hadron : ha.bHadrons()) {
//Compute branching ratios for listed b-hadrons
if (hadron_id(hadron.abspid()) != "") fill_Histos("b", hadron);
}
//c hadrons branching ratios
for (const Particle& hadron : ha.cHadrons()) {
if (!hadron.fromBottom()) { //take into account only c-hadrons that don't come from a b-hadron decay
//Compute branching ratios for listed c-hadrons
if (hadron_id(hadron.abspid()) != "") fill_Histos("c", hadron);
}
}
} // Close Event
/// Normalise histograms etc., after the run
void finalize() {
normalize(_h);
}
/// @}
private:
/// @name Histograms
/// @{
map<string, Histo1DPtr> _h;
/// @}
LorentzTransform _boost;
};
RIVET_DECLARE_PLUGIN(MC_HFBRANCHING);
}