00001 //---------------------------------------------------------------------- 00002 /// \file 00003 /// \page Example11 11 - boosted Higgs tagging 00004 /// 00005 /// fastjet example program, illustration of carrying out boosted 00006 /// Higgs subjet ID analysis 00007 /// 00008 /// It illustrates two kinds of functionality: 00009 /// 00010 /// - following the decomposition of a jet into pieces 00011 /// - following information on a b-tag through the jet 00012 /// 00013 /// This kind of functionality was used in arXiv:0802.2470 00014 /// (Butterworth, Davison, Rubin & Salam) for boosted Higgs searches, 00015 /// and related functionality was used in arXiv:0806.0848 (Kaplan, 00016 /// Rehermann, Schwartz & Tweedie) in searching for boosted tops 00017 /// (without b-tag assumptions). 00018 /// 00019 /// run it with : ./11-boosted_higgs < data/HZ-event-Hmass115.dat 00020 /// 00021 /// Source code: 11-boosted_higgs.cc 00022 //---------------------------------------------------------------------- 00023 00024 00025 //STARTHEADER 00026 // $Id: 11-boosted_higgs.cc 1911 2011-01-28 18:18:24Z soyez $ 00027 // 00028 // Copyright (c) 2005-2011, Matteo Cacciari, Gavin Salam and Gregory Soyez 00029 // 00030 //---------------------------------------------------------------------- 00031 // This file is part of FastJet. 00032 // 00033 // FastJet is free software; you can redistribute it and/or modify 00034 // it under the terms of the GNU General Public License as published by 00035 // the Free Software Foundation; either version 2 of the License, or 00036 // (at your option) any later version. 00037 // 00038 // The algorithms that underlie FastJet have required considerable 00039 // development and are described in hep-ph/0512210. If you use 00040 // FastJet as part of work towards a scientific publication, please 00041 // include a citation to the FastJet paper. 00042 // 00043 // FastJet is distributed in the hope that it will be useful, 00044 // but WITHOUT ANY WARRANTY; without even the implied warranty of 00045 // MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the 00046 // GNU General Public License for more details. 00047 // 00048 // You should have received a copy of the GNU General Public License 00049 // along with FastJet; if not, write to the Free Software 00050 // Foundation, Inc.: 00051 // 59 Temple Place, Suite 330, Boston, MA 02111-1307 USA 00052 //---------------------------------------------------------------------- 00053 //ENDHEADER 00054 00055 #include "fastjet/ClusterSequence.hh" 00056 #include <iostream> // needed for io 00057 #include <sstream> // needed for internal io 00058 #include <iomanip> 00059 #include <cmath> 00060 00061 using namespace std; 00062 using namespace fastjet; 00063 00064 00065 //---------------------------------------------------------------------- 00066 // set up a class to give standard (by default E-scheme) 00067 // recombination, with additional tracking of flavour information in 00068 // the user_index. 00069 // 00070 // If you use this, you must explicitly set the user index to 0 for 00071 // non-flavoured particles (the default value is -1); 00072 // 00073 // This will work for native algorithms, but not for all plugins 00074 //---------------------------------------------------------------------- 00075 typedef JetDefinition::DefaultRecombiner DefRecomb; 00076 00077 class FlavourRecombiner : public DefRecomb { 00078 public: 00079 FlavourRecombiner(RecombinationScheme recomb_scheme = E_scheme) : 00080 DefRecomb(recomb_scheme) {}; 00081 00082 virtual std::string description() const { 00083 return DefRecomb::description()+" (with user index addition)";} 00084 00085 /// recombine pa and pb and put result into pab 00086 virtual void recombine(const PseudoJet & pa, const PseudoJet & pb, 00087 PseudoJet & pab) const { 00088 DefRecomb::recombine(pa,pb,pab); 00089 pab.set_user_index(pa.user_index() + pb.user_index()); 00090 } 00091 }; 00092 00093 00094 //---------------------------------------------------------------------- 00095 // forward declaration for printing out info about a jet 00096 //---------------------------------------------------------------------- 00097 ostream & operator<<(ostream &, PseudoJet &); 00098 00099 00100 //---------------------------------------------------------------------- 00101 // core of the program 00102 //---------------------------------------------------------------------- 00103 int main (int argc, char ** argv) { 00104 00105 vector<PseudoJet> particles; 00106 00107 // read in data in format px py pz E b-tag [last of these is optional] 00108 // lines starting with "#" are considered as comments and discarded 00109 //---------------------------------------------------------- 00110 00111 string line; 00112 while (getline(cin,line)) { 00113 if (line.substr(0,1) == "#") {continue;} 00114 istringstream linestream(line); 00115 double px,py,pz,E; 00116 linestream >> px >> py >> pz >> E; 00117 00118 // optionally read in btag information 00119 int btag; 00120 if (! (linestream >> btag)) btag = 0; 00121 00122 // construct the particle 00123 PseudoJet particle(px,py,pz,E); 00124 particle.set_user_index(btag); // btag info goes in user index, for flavour tracking 00125 particles.push_back(particle); 00126 } 00127 00128 00129 // set up the jet finding 00130 // 00131 // This also shows how to use the "FlavourRecombiner" user-defined 00132 // recombiner 00133 // ---------------------------------------------------------- 00134 double R = 1.2; 00135 FlavourRecombiner flav_recombiner; // for tracking flavour 00136 JetDefinition jet_def(cambridge_algorithm, R, &flav_recombiner); 00137 00138 00139 // run the jet finding; find the hardest jet 00140 ClusterSequence cs(particles, jet_def); 00141 vector<PseudoJet> jets = sorted_by_pt(cs.inclusive_jets()); 00142 00143 cout << "Ran: " << jet_def.description() << endl << endl; 00144 cout << "Hardest jet: " << jets[0] << endl << endl; 00145 00146 // now do the subjet decomposition 00147 //---------------------------------------------------------- 00148 // 00149 // when unpeeling a C/A jet, often only a very soft piece may break off; 00150 // the mass_drop_threshold indicates how much "lighter" the heavier of the two 00151 // resulting pieces must be in order for us to consider that we've really 00152 // seen some form of substructure 00153 double mass_drop_threshold = 0.667; 00154 // QCD backgrounds that give larger jet masses have a component 00155 // where a quite soft gluon is emitted; to eliminate part of this 00156 // one can place a cut on the asymmetry of the branching; 00157 // 00158 // Here the cut is expressed in terms of y, the kt-distance scaled 00159 // to the squared jet mass; an easier way to see it is in terms of 00160 // a requirement on the momentum fraction in the splitting: z/(1-z) 00161 // and (1-z)/z > rtycut^2 [the correspondence holds only at LO] 00162 double rtycut = 0.3; 00163 00164 PseudoJet this_jet = jets[0]; 00165 PseudoJet parent1, parent2; 00166 bool had_parents; 00167 00168 while ((had_parents = this_jet.has_parents(parent1,parent2))) { 00169 // make parent1 the more massive jet 00170 if (parent1.m() < parent2.m()) swap(parent1,parent2); 00171 00172 // if we pass the conditions on the mass drop and its degree of 00173 // asymmetry (z/(1-z) \sim kt_dist/m^2 > rtycut), then we've found 00174 // something interesting, so exit the loop 00175 if (parent1.m() < mass_drop_threshold * this_jet.m() && 00176 parent1.kt_distance(parent2) > pow(rtycut,2) * this_jet.m2()) { 00177 break; 00178 } else { 00179 // otherwise try a futher decomposition on the more massive jet 00180 this_jet = parent1; 00181 } 00182 } 00183 00184 // look to see what we found 00185 if (!had_parents) { 00186 cout << "Did not find suitable hard substructure in this event." << endl; 00187 return 0; 00188 } 00189 00190 cout << "Found suitable pair of subjets: " << endl; 00191 cout << " " << parent1 << endl; 00192 cout << " " << parent2 << endl; 00193 cout << "Total = " << endl; 00194 cout << " " << this_jet << endl << endl; 00195 00196 // next we "filter" it, to remove UE & pileup contamination 00197 //---------------------------------------------------------- 00198 // 00199 // [there are two ways of doing this; here we directly use the 00200 // exsiting cluster sequence and find the exclusive subjets of 00201 // this_jet (i.e. work backwards within the cs starting from 00202 // this_jet); alternatively one can recluster just the 00203 // constituents of the jet] 00204 // 00205 // first get separation between the subjets (called Rbb -- assuming it's a Higgs!) 00206 double Rbb = sqrt(parent1.squared_distance(parent2)); 00207 double Rfilt = min(Rbb/2, 0.3); // somewhat arbitrary choice 00208 unsigned nfilt = 3; // number of pieces we'll take 00209 cout << "Subjet separation (Rbb) = " << Rbb << ", Rfilt = " << Rfilt << endl; 00210 00211 double dcut = pow(Rfilt/R,2); // for C/A get a view at Rfilt by 00212 // using a dcut=(Rfilt/R)^2 00213 vector<PseudoJet> filt_subjets = sorted_by_pt(this_jet.exclusive_subjets(dcut)); 00214 00215 // now print out the filtered jets and reconstruct total 00216 // at the same time 00217 cout << "Filtered pieces are " << endl; 00218 cout << " " << filt_subjets[0] << endl; 00219 PseudoJet filtered_total = filt_subjets[0]; 00220 for (unsigned i = 1; i < nfilt && i < filt_subjets.size(); i++) { 00221 cout << " " << filt_subjets[i] << endl; 00222 flav_recombiner.plus_equal(filtered_total, filt_subjets[i]); 00223 } 00224 cout << "Filtered total is " << endl; 00225 cout << " " << filtered_total << endl; 00226 00227 } 00228 00229 00230 //---------------------------------------------------------------------- 00231 // does the actual work for printing out a jet 00232 //---------------------------------------------------------------------- 00233 ostream & operator<<(ostream & ostr, PseudoJet & jet) { 00234 ostr << "pt, y, phi =" 00235 << " " << setw(10) << jet.perp() 00236 << " " << setw(6) << jet.rap() 00237 << " " << setw(6) << jet.phi() 00238 << ", mass = " << setw(10) << jet.m() 00239 << ", btag = " << jet.user_index(); 00240 return ostr; 00241 }