[d7d2da3] | 1 | // -*- C++ -*-
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| 2 | ///////////////////////////////////////////////////////////////////////////////
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| 3 | // File: area.h //
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| 4 | // Description: header file for the computation of jet area //
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| 5 | // This file is part of the SISCone project. //
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| 6 | // For more details, see http://projects.hepforge.org/siscone //
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| 7 | // //
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| 8 | // Copyright (c) 2006 Gavin Salam and Gregory Soyez //
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| 9 | // //
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| 10 | // This program is free software; you can redistribute it and/or modify //
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| 11 | // it under the terms of the GNU General Public License as published by //
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| 12 | // the Free Software Foundation; either version 2 of the License, or //
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| 13 | // (at your option) any later version. //
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| 14 | // //
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| 15 | // This program is distributed in the hope that it will be useful, //
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| 16 | // but WITHOUT ANY WARRANTY; without even the implied warranty of //
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| 17 | // MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the //
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| 18 | // GNU General Public License for more details. //
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| 19 | // //
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| 20 | // You should have received a copy of the GNU General Public License //
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| 21 | // along with this program; if not, write to the Free Software //
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| 22 | // Foundation, Inc., 51 Franklin St, Fifth Floor, Boston, MA 02110-1301, USA //
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| 23 | // //
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[35cdc46] | 24 | // $Revision:: 149 $//
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| 25 | // $Date:: 2007-03-15 00:13:58 +0100 (Thu, 15 Mar 2007) $//
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[d7d2da3] | 26 | ///////////////////////////////////////////////////////////////////////////////
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| 27 |
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| 28 | #include "area.h"
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| 29 | #include "momentum.h"
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| 30 | #include <stdlib.h>
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| 31 | #include <iostream>
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| 32 |
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| 33 | namespace siscone{
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| 34 | using namespace std;
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| 35 |
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| 36 | /*******************************************************
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| 37 | * Cjet_area implementation *
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| 38 | * real Jet information, including its area(s) *
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| 39 | * *
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| 40 | * This class contains information for one single jet. *
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| 41 | * That is, first, its momentum carrying information *
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| 42 | * about its centre and pT, and second, its particle *
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| 43 | * contents (from CJeT). *
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| 44 | * Compared to the Cjet class, it also includes the *
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| 45 | * passive and active areas of the jet computed using *
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| 46 | * the Carea class. *
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| 47 | *******************************************************/
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| 48 |
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| 49 | // default ctor
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| 50 | //--------------
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| 51 | Cjet_area::Cjet_area(){
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| 52 | active_area = passive_area = 0.0;
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| 53 | }
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| 54 |
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| 55 | // jet-initiated ctor
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| 56 | //-------------------
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| 57 | Cjet_area::Cjet_area(Cjet &j){
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| 58 | v = j.v;
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| 59 | n = j.n;
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| 60 | contents = j.contents;
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| 61 |
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| 62 | pass = j.pass;
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| 63 |
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| 64 | pt_tilde = j.pt_tilde;
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| 65 | sm_var2 = j.sm_var2;
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| 66 |
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| 67 | active_area = passive_area = 0.0;
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| 68 | }
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| 69 |
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| 70 | // default dtor
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| 71 | //--------------
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| 72 | Cjet_area::~Cjet_area(){
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| 73 |
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| 74 | }
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| 75 |
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| 76 |
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| 77 | /******************************************************************
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| 78 | * Csiscone_area implementation *
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| 79 | * class for the computation of jet areas. *
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| 80 | * *
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| 81 | * This is the class user should use whenever you want to compute *
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| 82 | * the jet area (passive and active). *
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| 83 | * It uses the SISCone algorithm to perform the jet analysis. *
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| 84 | ******************************************************************/
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| 85 |
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| 86 | // default ctor
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| 87 | //-------------
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| 88 | Carea::Carea(){
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| 89 | grid_size = 60; // 3600 particles added
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| 90 | grid_eta_max = 6.0; // maybe having twice more points in eta than in phi should be nice
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| 91 | grid_shift = 0.5; // 50% "shacking"
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| 92 |
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| 93 | pt_soft = 1e-100;
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| 94 | pt_shift = 0.05;
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| 95 | pt_soft_min = 1e-90;
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| 96 | }
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| 97 |
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| 98 | // default dtor
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| 99 | //-------------
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| 100 | Carea::~Carea(){
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| 101 |
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| 102 | }
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| 103 |
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| 104 | /*
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| 105 | * compute the jet areas from a given particle set.
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| 106 | * The parameters of this method are the ones which control the jet clustering alghorithm.
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| 107 | * Note that the pt_min is not allowed here soince the jet-area determination involves soft
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| 108 | * particles/jets and thus is used internally.
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| 109 | * - _particles list of particles
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| 110 | * - _radius cone radius
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| 111 | * - _f shared energy threshold for splitting&merging
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| 112 | * - _n_pass_max maximum number of passes (0=full search, the default)
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| 113 | * - _split_merge_scale the scale choice for the split-merge procedure
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| 114 | * NOTE: SM_pt leads to IR unsafety for some events with momentum conservation.
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| 115 | * SM_Et is IR safe but not boost invariant and not implemented(!)
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| 116 | * SM_mt is IR safe for hadronic events, but not for decays of two
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| 117 | * back-to-back particles of identical mass
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| 118 | * SM_pttilde
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| 119 | * is always IR safe, and also boost invariant (default)
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| 120 | * - _hard_only when this is set on, only hard jets are computed
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| 121 | * and not the purely ghosted jets (default: false)
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| 122 | * return the jets together with their areas
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| 123 | * The return value is the number of jets (including pure-ghost ones if they are included)
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| 124 | ********************************************************************************************/
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| 125 | int Carea::compute_areas(std::vector<Cmomentum> &_particles, double _radius, double _f,
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| 126 | int _n_pass_max, Esplit_merge_scale _split_merge_scale,
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| 127 | bool _hard_only){
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| 128 |
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| 129 | vector<Cmomentum> all_particles;
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| 130 |
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| 131 | // put "hardest cut-off" if needed
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| 132 | // this avoids computation of ghosted jets when not required and
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| 133 | // significantly shortens the SM.
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| 134 | if (_hard_only){
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| 135 | SM_var2_hardest_cut_off = pt_soft_min*pt_soft_min;
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| 136 | }
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| 137 |
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| 138 | // clear potential previous runs
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| 139 | jet_areas.clear();
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| 140 |
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| 141 | // put initial set of particles in the list
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| 142 | int n_hard = _particles.size();
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| 143 | all_particles = _particles;
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| 144 |
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| 145 | // build the set of ghost particles and add them to the particle list
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| 146 | int i,j;
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| 147 | double eta_g,phi_g,pt_g;
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| 148 |
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| 149 | for (i=0;i<grid_size;i++){
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| 150 | for (j=0;j<grid_size;j++){
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| 151 | eta_g = grid_eta_max*(-1.0+2.0*(i+0.5+grid_shift*(-1.0+2.0*(rand()/(RAND_MAX+1.0))))/grid_size);
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| 152 | phi_g = M_PI *(-1.0+2.0*(j+0.5+grid_shift*(-1.0+2.0*(rand()/(RAND_MAX+1.0))))/grid_size);
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| 153 | pt_g = pt_soft*(1.0+pt_shift*(-1.0+2.0*(rand()/(RAND_MAX+1.0))));
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| 154 | all_particles.push_back(Cmomentum(pt_g*cos(phi_g),pt_g*sin(phi_g),pt_g*sinh(eta_g),pt_g*cosh(eta_g)));
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| 155 | }
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| 156 | }
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| 157 |
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| 158 | // run clustering with all particles.
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| 159 | // the split-merge here dynamically accounts for the purely soft jets.
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| 160 | // we therefore end up with the active area for the jets
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| 161 | int n_jets = compute_jets(all_particles, _radius, _f, _n_pass_max, 0.0, _split_merge_scale);
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| 162 |
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| 163 | // save jets in the Cjet_area structure
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| 164 | // and determine their size
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| 165 | // jet contents is ordered by increasing index of the initial
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| 166 | // particles. Hence, we look for the first particle with index >= n_hard
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| 167 | // and deduce the number of ghosts in the jet, hence the area.
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| 168 | double area_factor = (2.0*grid_eta_max/grid_size)*(twopi/grid_size);
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| 169 |
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| 170 | for (i=0;i<(int) jets.size();i++){
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| 171 | jet_areas.push_back(jets[i]);
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| 172 | j=0;
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| 173 | while ((j<jets[i].n) && (jets[i].contents[j]<n_hard)) j++;
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| 174 | jet_areas[i].active_area = (jets[i].n-j)*area_factor;
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| 175 | }
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| 176 |
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| 177 | // determine passive jet area
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| 178 | // for that onem we use the pt_min cut in order to remove purely
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| 179 | // soft jets from the SM procedure
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| 180 | recompute_jets(_f, pt_soft_min);
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| 181 |
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| 182 | // for the area computation, we assume the jete order is the same!
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| 183 | for (i=0;i<(int) jets.size();i++){
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| 184 | j=0;
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| 185 | while ((j<jets[i].n) && (jets[i].contents[j]<n_hard)) j++;
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| 186 | jet_areas[i].passive_area = (jets[i].n-j)*area_factor;
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| 187 | }
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| 188 |
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| 189 | // Note:
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| 190 | // there surely remain purely soft je at the end
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| 191 | // their active area is 0 by default (see ctor)
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| 192 |
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| 193 | jets.clear();
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| 194 |
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| 195 | return n_jets;
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| 196 | }
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| 197 |
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| 198 | /*
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| 199 | * compute the passive jet areas from a given particle set.
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| 200 | * The parameters of this method are the ones which control the jet clustering alghorithm.
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| 201 | * Note that the pt_min is not allowed here soince the jet-area determination involves soft
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| 202 | * particles/jets and thus is used internally.
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| 203 | * - _particles list of particles
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| 204 | * - _radius cone radius
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| 205 | * - _f shared energy threshold for splitting&merging
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| 206 | * - _n_pass_max maximum number of passes (0=full search, the default)
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| 207 | * - _split_merge_scale the scale choice for the split-merge procedure
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| 208 | * NOTE: SM_pt leads to IR unsafety for some events with momentum conservation.
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| 209 | * SM_Et is IR safe but not boost invariant and not implemented(!)
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| 210 | * SM_mt is IR safe for hadronic events, but not for decays of two
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| 211 | * back-to-back particles of identical mass
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| 212 | * SM_pttilde
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| 213 | * is always IR safe, and also boost invariant (default)
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| 214 | * return the jets together with their passive areas
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| 215 | * The return value is the number of jets
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| 216 | ********************************************************************************************/
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| 217 | int Carea::compute_passive_areas(std::vector<Cmomentum> &_particles, double _radius, double _f,
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| 218 | int _n_pass_max, Esplit_merge_scale _split_merge_scale){
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| 219 |
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| 220 | vector<Cmomentum> all_particles;
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| 221 |
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| 222 | // in the case of passive area, we do not need
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| 223 | // to put the ghosts in the stable-cone search
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| 224 | // (they do no influence the list of stable cones)
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| 225 | // Here's how it goes...
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| 226 | stable_cone_soft_pt2_cutoff = pt_soft_min*pt_soft_min;
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| 227 |
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| 228 | // clear potential previous runs
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| 229 | jet_areas.clear();
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| 230 |
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| 231 | // put initial set of particles in the list
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| 232 | int n_hard = _particles.size();
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| 233 | all_particles = _particles;
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| 234 |
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| 235 | // build the set of ghost particles and add them to the particle list
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| 236 | int i,j;
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| 237 | double eta_g,phi_g,pt_g;
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| 238 |
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| 239 | for (i=0;i<grid_size;i++){
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| 240 | for (j=0;j<grid_size;j++){
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| 241 | eta_g = grid_eta_max*(-1.0+2.0*(i+0.5+grid_shift*(-1.0+2.0*(rand()/(RAND_MAX+1.0))))/grid_size);
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| 242 | phi_g = M_PI *(-1.0+2.0*(j+0.5+grid_shift*(-1.0+2.0*(rand()/(RAND_MAX+1.0))))/grid_size);
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| 243 | pt_g = pt_soft*(1.0+pt_shift*(-1.0+2.0*(rand()/(RAND_MAX+1.0))));
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| 244 | all_particles.push_back(Cmomentum(pt_g*cos(phi_g),pt_g*sin(phi_g),pt_g*sinh(eta_g),pt_g*cosh(eta_g)));
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| 245 | }
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| 246 | }
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| 247 |
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| 248 | // determine passive jet area
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| 249 | // for that onem we use the pt_min cut in order to remove purely
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| 250 | // soft jets from the SM procedure
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| 251 | int n_jets = compute_jets(all_particles, _radius, _f, _n_pass_max, pt_soft_min, _split_merge_scale);
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| 252 |
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| 253 | // save jets in the Cjet_area structure
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| 254 | // and determine their size
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| 255 | // jet contents is ordered by increasing index of the initial
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| 256 | // particles. Hence, we look for the first particle with index >= n_hard
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| 257 | // and deduce the number of ghosts in the jet, hence the area.
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| 258 | double area_factor = (2.0*grid_eta_max/grid_size)*(twopi/grid_size);
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| 259 | for (i=0;i<(int) jets.size();i++){
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| 260 | j=0;
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| 261 | while ((j<jets[i].n) && (jets[i].contents[j]<n_hard)) j++;
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| 262 | jet_areas[i].passive_area = (jets[i].n-j)*area_factor;
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| 263 | }
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| 264 |
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| 265 | jets.clear();
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| 266 |
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| 267 | return n_jets;
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| 268 | }
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| 269 |
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| 270 | /*
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| 271 | * compute the active jet areas from a given particle set.
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| 272 | * The parameters of this method are the ones which control the jet clustering alghorithm.
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| 273 | * Note that the pt_min is not allowed here soince the jet-area determination involves soft
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| 274 | * particles/jets and thus is used internally.
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| 275 | * - _particles list of particles
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| 276 | * - _radius cone radius
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| 277 | * - _f shared energy threshold for splitting&merging
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| 278 | * - _n_pass_max maximum number of passes (0=full search, the default)
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| 279 | * - _split_merge_scale the scale choice for the split-merge procedure
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| 280 | * NOTE: SM_pt leads to IR unsafety for some events with momentum conservation.
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| 281 | * SM_Et is IR safe but not boost invariant and not implemented(!)
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| 282 | * SM_mt is IR safe for hadronic events, but not for decays of two
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| 283 | * back-to-back particles of identical mass
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| 284 | * SM_pttilde
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| 285 | * is always IR safe, and also boost invariant (default)
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| 286 | * - _hard_only when this is set on, only hard jets are computed
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| 287 | * and not the purely ghosted jets (default: false)
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| 288 | * return the jets together with their active areas
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| 289 | * The return value is the number of jets (including pure-ghost ones if they are included)
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| 290 | ********************************************************************************************/
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| 291 | int Carea::compute_active_areas(std::vector<Cmomentum> &_particles, double _radius, double _f,
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| 292 | int _n_pass_max, Esplit_merge_scale _split_merge_scale,
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| 293 | bool _hard_only){
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| 294 |
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| 295 | vector<Cmomentum> all_particles;
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| 296 |
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| 297 | // put "hardest cut-off" if needed
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| 298 | // this avoids computation of ghosted jets when not required and
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| 299 | // significantly shortens the SM.
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| 300 | if (_hard_only){
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| 301 | SM_var2_hardest_cut_off = pt_soft_min*pt_soft_min;
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| 302 | }
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| 303 |
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| 304 | // clear potential previous runs
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| 305 | jet_areas.clear();
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| 306 |
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| 307 | // put initial set of particles in the list
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| 308 | int n_hard = _particles.size();
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| 309 | all_particles = _particles;
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| 310 |
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| 311 | // build the set of ghost particles and add them to the particle list
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| 312 | int i,j;
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| 313 | double eta_g,phi_g,pt_g;
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| 314 |
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| 315 | for (i=0;i<grid_size;i++){
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| 316 | for (j=0;j<grid_size;j++){
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| 317 | eta_g = grid_eta_max*(-1.0+2.0*(i+0.5+grid_shift*(-1.0+2.0*(rand()/(RAND_MAX+1.0))))/grid_size);
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| 318 | phi_g = M_PI *(-1.0+2.0*(j+0.5+grid_shift*(-1.0+2.0*(rand()/(RAND_MAX+1.0))))/grid_size);
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| 319 | pt_g = pt_soft*(1.0+pt_shift*(-1.0+2.0*(rand()/(RAND_MAX+1.0))));
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| 320 | all_particles.push_back(Cmomentum(pt_g*cos(phi_g),pt_g*sin(phi_g),pt_g*sinh(eta_g),pt_g*cosh(eta_g)));
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| 321 | }
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| 322 | }
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| 323 |
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| 324 | // run clustering with all particles.
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| 325 | // the split-merge here dynamically accounts for the purely soft jets.
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| 326 | // we therefore end up with the active area for the jets
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| 327 | int n_jets = compute_jets(all_particles, _radius, _f, _n_pass_max, 0.0, _split_merge_scale);
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| 328 |
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| 329 | // save jets in the Cjet_area structure
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| 330 | // and determine their size
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| 331 | // jet contents is ordered by increasing index of the initial
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| 332 | // particles. Hence, we look for the first particle with index >= n_hard
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| 333 | // and deduce the number of ghosts in the jet, hence the area.
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| 334 | double area_factor = (2.0*grid_eta_max/grid_size)*(twopi/grid_size);
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| 335 |
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| 336 | for (i=0;i<(int) jets.size();i++){
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| 337 | jet_areas.push_back(jets[i]);
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| 338 | j=0;
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| 339 | while ((j<jets[i].n) && (jets[i].contents[j]<n_hard)) j++;
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| 340 | jet_areas[i].active_area = (jets[i].n-j)*area_factor;
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| 341 | }
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| 342 |
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| 343 | jets.clear();
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| 344 |
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| 345 | return n_jets;
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| 346 | }
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| 347 |
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| 348 | }
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