[d7d2da3] | 1 | // -*- C++ -*-
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| 2 | ///////////////////////////////////////////////////////////////////////////////
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| 3 | // File: split_merge.h //
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| 4 | // Description: header file for splitting/merging (contains the CJet class) //
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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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[1d208a2] | 24 | // $Revision:: 405 $//
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| 25 | // $Date:: 2016-05-23 20:15:02 +0200 (Mon, 23 May 2016) $//
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[d7d2da3] | 26 | ///////////////////////////////////////////////////////////////////////////////
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| 27 |
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| 28 | #ifndef __SPLIT_MERGE_H__
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| 29 | #define __SPLIT_MERGE_H__
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| 30 |
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[1d208a2] | 31 | #include "config.h"
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[d7d2da3] | 32 | #include "defines.h"
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| 33 | #include "geom_2d.h"
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| 34 | #include "momentum.h"
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| 35 | #include <stdio.h>
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| 36 | #include <vector>
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| 37 | #include <set>
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| 38 | #include <memory>
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| 39 | #include <string>
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| 40 |
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| 41 | namespace siscone{
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| 42 |
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[1d208a2] | 43 | const int CJET_INEXISTENT_PASS = -2;
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| 44 |
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[d7d2da3] | 45 | /**
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| 46 | * \class Cjet
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| 47 | * real Jet information.
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| 48 | *
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| 49 | * This class contains information for one single jet.
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| 50 | * That is, first, its momentum carrying information
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| 51 | * about its centre and pT, and second, its particle
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| 52 | * contents
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| 53 | */
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| 54 | class Cjet{
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| 55 | public:
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| 56 | /// default ctor
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| 57 | Cjet();
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| 58 |
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| 59 | /// default dtor
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| 60 | ~Cjet();
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| 61 |
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| 62 | Cmomentum v; ///< jet momentum
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| 63 | double pt_tilde; ///< p-scheme pt
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| 64 | int n; ///< number of particles inside
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| 65 | std::vector<int> contents; ///< particle contents (list of indices)
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| 66 |
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| 67 | /// ordering variable used for ordering and overlap in the
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| 68 | /// split--merge. This variable is automatically set either to
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| 69 | /// pt_tilde, or to mt or to pt, depending on the siscone
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| 70 | /// parameter. Note that the default behaviour is pt_tilde and that
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| 71 | /// other chices may lead to infrared unsafe situations.
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| 72 | /// Note: we use the square of the varible rather than the variable itself
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| 73 | double sm_var2;
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| 74 |
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| 75 | /// covered range in eta-phi
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| 76 | Ceta_phi_range range;
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| 77 |
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| 78 | /// pass at which the jet has been found
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| 79 | /// It starts at 0 (first pass), -1 means infinite rapidity
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[1d208a2] | 80 | /// (it will be initialised to "CJET_INEXISTENT_PASS" which should
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| 81 | /// never appear after clustering)
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[d7d2da3] | 82 | int pass;
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| 83 | };
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| 84 |
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| 85 | /// ordering of jets in pt (e.g. used in final jets ordering)
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| 86 | bool jets_pt_less(const Cjet &j1, const Cjet &j2);
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| 87 |
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| 88 |
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| 89 | /// the choices of scale variable that can be used in the split-merge
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| 90 | /// step, both for ordering the protojets and for measuing their
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| 91 | /// overlap; pt, Et and mt=sqrt(pt^2+m^2) are all defined in E-scheme
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| 92 | /// (4-momentum) recombination; pttilde = \sum_{i\in jet} |p_{t,i}|
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| 93 | ///
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| 94 | /// NB: if one changes the order here, one _MUST_ also change the order
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| 95 | /// in the SISCone plugin
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| 96 | enum Esplit_merge_scale {
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| 97 | SM_pt, ///< transverse momentum (E-scheme), IR unsafe
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| 98 | SM_Et, ///< transverse energy (E-scheme), not long. boost inv.
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| 99 | ///< original run-II choice [may not be implemented]
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| 100 | SM_mt, ///< transverse mass (E-scheme), IR safe except
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| 101 | ///< in decays of two identical narrow heavy particles
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| 102 | SM_pttilde ///< pt-scheme pt = \sum_{i in jet} |p_{ti}|, should
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| 103 | ///< be IR safe in all cases
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| 104 | };
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| 105 |
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| 106 | /// return the name of the split-merge scale choice
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| 107 | std::string split_merge_scale_name(Esplit_merge_scale sms);
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| 108 |
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| 109 | /**
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| 110 | * \class Csplit_merge_ptcomparison
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| 111 | * comparison of jets for split--merge ordering
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| 112 | *
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| 113 | * a class that allows us to carry out comparisons of pt of jets, using
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| 114 | * information from exact particle contents where necessary.
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| 115 | */
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| 116 | class Csplit_merge_ptcomparison{
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| 117 | public:
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| 118 | /// default ctor
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| 119 | Csplit_merge_ptcomparison() :
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| 120 | particles(0), split_merge_scale(SM_pttilde){};
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| 121 |
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| 122 | /// return the name corresponding to the SM scale variable
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| 123 | std::string SM_scale_name() const {
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| 124 | return split_merge_scale_name(split_merge_scale);}
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| 125 |
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| 126 | std::vector<Cmomentum> * particles; ///< pointer to the list of particles
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| 127 | std::vector<double> * pt; ///< pointer to the pt of the particles
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| 128 |
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| 129 | /// comparison between 2 jets
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| 130 | bool operator()(const Cjet &jet1, const Cjet &jet2) const;
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| 131 |
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| 132 | /**
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| 133 | * get the difference between 2 jets, calculated such that rounding
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| 134 | * errors will not affect the result even if the two jets have
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| 135 | * almost the same content (so that the difference is below the
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| 136 | * rounding errors)
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| 137 | *
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| 138 | * \param j1 first jet
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| 139 | * \param j2 second jet
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| 140 | * \param v jet1-jet2
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| 141 | * \param pt_tilde jet1-jet2 pt_tilde
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| 142 | */
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| 143 | void get_difference(const Cjet &j1, const Cjet &j2, Cmomentum *v, double *pt_tilde) const;
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| 144 |
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| 145 | /// the following parameter controls the variable we're using for
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| 146 | /// the split-merge process i.e. the variable we use for
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| 147 | /// 1. ordering jet candidates;
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[273e668] | 148 | /// 2. computing the overlap fraction of two candidates.
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[d7d2da3] | 149 | /// The default value uses pttile (p-scheme pt). Other alternatives are
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| 150 | /// pt, mt=sqrt(pt^2+m^2)=sqrt(E^2-pz^2) or Et.
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| 151 | /// NOTE: Modifying the default choice can have nasty effects:
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| 152 | /// - using pt leads to some IR unsafety when we have two jets,
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| 153 | /// e.g. back-to-back, with the same pt. In that case, their ordering
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| 154 | /// in pt is random and can be affected by the addition of a
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| 155 | /// soft particle. Hence, we highly recommand to keep this to
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| 156 | /// the default value i.e. to use pt only for the purpose of
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| 157 | /// investigating the IR issue
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[273e668] | 158 | /// - using Et is safe but does not respect boost invariance
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[d7d2da3] | 159 | /// - using mt solves the IR unsafety issues with the pt variable
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| 160 | /// for QCD jets but the IR unsafety remains for nack-to-back
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| 161 | /// jets of unstable narrow-width particles (e.g. Higgs).
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| 162 | /// Therefore, keeping the default value is strongly advised.
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| 163 | Esplit_merge_scale split_merge_scale;
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| 164 | };
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| 165 |
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| 166 |
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| 167 | // iterator types
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| 168 | /// iterator definition for the jet candidates structure
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| 169 | typedef std::multiset<siscone::Cjet,Csplit_merge_ptcomparison>::iterator cjet_iterator;
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| 170 |
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| 171 | /// iterator definition for the jet structure
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| 172 | typedef std::vector<siscone::Cjet>::iterator jet_iterator;
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| 173 |
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| 174 |
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| 175 |
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| 176 | /**
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| 177 | * \class Csplit_merge
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| 178 | * Class used to split and merge jets.
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| 179 | */
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| 180 | class Csplit_merge{
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| 181 | public:
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| 182 | /// default ctor
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| 183 | Csplit_merge();
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| 184 |
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| 185 | /// default dtor
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| 186 | ~Csplit_merge();
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| 187 |
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| 188 |
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| 189 | //////////////////////////////
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| 190 | // initialisation functions //
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| 191 | //////////////////////////////
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| 192 |
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| 193 | /**
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| 194 | * initialisation function
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| 195 | * \param _particles list of particles
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| 196 | * \param protocones list of protocones (initial jet candidates)
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| 197 | * \param R2 cone radius (squared)
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| 198 | * \param ptmin minimal pT allowed for jets
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| 199 | * \return 0 on success, 1 on error
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| 200 | */
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| 201 | int init(std::vector<Cmomentum> &_particles, std::vector<Cmomentum> *protocones, double R2, double ptmin=0.0);
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| 202 |
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| 203 | /**
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| 204 | * initialisation function for particle list
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| 205 | * \param _particles list of particles
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| 206 | * \return 0 on success, 1 on error
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| 207 | */
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| 208 | int init_particles(std::vector<Cmomentum> &_particles);
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| 209 |
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| 210 | /**
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| 211 | * build initial list of left particles
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| 212 | */
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| 213 | int init_pleft();
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| 214 |
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| 215 | /**
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| 216 | * use a pt-dependent boundary for splitting
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| 217 | * When called with true, the criterium for splitting two protojets
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| 218 | * will be to compare D1^2/kt1^2 vs. D2^2/kt2^2, the (anti-)kt-weighted
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| 219 | * distance instead of the plain distance D1^2 vs. D2^2.
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| 220 | * This can be set in order to produce more circular hard jets,
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| 221 | * with the same underlying philosophy as for the anti-kt algorithm.
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| 222 | * We thus expect a behaviour closer to the IterativeCone one.
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| 223 | * By default, we use the standard D1^2 vs. D2^2 comparison and this
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| 224 | * function is not called.
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| 225 | */
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| 226 | inline int set_pt_weighted_splitting(bool _use_pt_weighted_splitting){
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| 227 | use_pt_weighted_splitting = _use_pt_weighted_splitting;
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| 228 | return 0;
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| 229 | }
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| 230 |
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| 231 | ////////////////////////
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| 232 | // cleaning functions //
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| 233 | ////////////////////////
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| 234 |
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| 235 | /// partial clearance
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| 236 | int partial_clear();
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| 237 |
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| 238 | /// full clearance
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| 239 | int full_clear();
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| 240 |
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[273e668] | 241 | ///////////////////////////////////////
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| 242 | // user-defined stable-cone ordering //
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| 243 | ///////////////////////////////////////
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| 244 |
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| 245 | /// \class Cuser_scale_base
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| 246 | /// base class for user-defined ordering of stable cones
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| 247 | ///
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| 248 | /// derived classes have to implement the () operator that returns
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| 249 | /// the scale associated with a given jet.
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| 250 | class Cuser_scale_base{
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| 251 | public:
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| 252 | /// empty virtual dtor
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| 253 | virtual ~Cuser_scale_base(){}
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| 254 |
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| 255 | /// the scale associated with a given jet
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| 256 | ///
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| 257 | /// "progressive removal" iteratively removes the stable cone with
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| 258 | /// the largest scale
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| 259 | virtual double operator()(const Cjet & jet) const = 0;
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| 260 |
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| 261 | /// returns true when the scale associated with jet a is larger than
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| 262 | /// the scale associated with jet b
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| 263 | ///
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| 264 | /// By default this does a simple direct comparison but it can be
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| 265 | /// overloaded for higher precision [recommended if possible]
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| 266 | ///
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| 267 | /// This function assumes that a.sm_var2 and b.sm_var2 have been
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| 268 | /// correctly initialised with the signed squared output of
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| 269 | /// operator(), as is by default the case when is_larger is called
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| 270 | /// from within siscone.
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| 271 | virtual bool is_larger(const Cjet & a, const Cjet & b) const{
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| 272 | return (a.sm_var2 > b.sm_var2);
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| 273 | }
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| 274 | };
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| 275 |
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| 276 | /// associate a user-defined scale to order the stable cones
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| 277 | ///
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| 278 | /// Note that this is only used in "progressive-removal mode",
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| 279 | /// e.g. in add_hardest_protocone_to_jets().
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| 280 | void set_user_scale(const Cuser_scale_base * user_scale_in){
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| 281 | _user_scale = user_scale_in;
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| 282 | }
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| 283 |
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| 284 | /// return the user-defined scale (NULL if none)
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| 285 | const Cuser_scale_base * user_scale() const { return _user_scale; }
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| 286 |
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[d7d2da3] | 287 |
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| 288 | /////////////////////////////////
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| 289 | // main parts of the algorithm //
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| 290 | /////////////////////////////////
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| 291 |
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| 292 | /**
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| 293 | * build the list 'p_uncol_hard' from p_remain by clustering
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| 294 | * collinear particles and removing particles softer than
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| 295 | * stable_cone_soft_pt2_cutoff
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| 296 | * note that thins in only used for stable-cone detection
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| 297 | * so the parent_index field is unnecessary
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| 298 | */
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| 299 | int merge_collinear_and_remove_soft();
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| 300 |
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| 301 | /**
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| 302 | * add a list of protocones
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| 303 | * \param protocones list of protocones (initial jet candidates)
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| 304 | * \param R2 cone radius (squared)
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| 305 | * \param ptmin minimal pT allowed for jets
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| 306 | * \return 0 on success, 1 on error
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| 307 | */
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| 308 | int add_protocones(std::vector<Cmomentum> *protocones, double R2, double ptmin=0.0);
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| 309 |
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[273e668] | 310 | /**
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| 311 | * remove the hardest protocone and declare it a jet
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| 312 | * \param protocones list of protocones (initial jet candidates)
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| 313 | * \param R2 cone radius (squared)
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| 314 | * \param ptmin minimal pT allowed for jets
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| 315 | * \return 0 on success, 1 on error
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| 316 | *
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| 317 | * The list of remaining particles (and the uncollinear-hard ones)
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| 318 | * is updated.
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| 319 | */
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| 320 | int add_hardest_protocone_to_jets(std::vector<Cmomentum> *protocones, double R2, double ptmin=0.0);
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| 321 |
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[d7d2da3] | 322 | /**
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| 323 | * really do the splitting and merging
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| 324 | * At the end, the vector jets is filled with the jets found.
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| 325 | * the 'contents' field of each jets contains the indices
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| 326 | * of the particles included in that jet.
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| 327 | * \param overlap_tshold threshold for splitting/merging transition
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| 328 | * \param ptmin minimal pT allowed for jets
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| 329 | * \return the number of jets is returned
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| 330 | */
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| 331 | int perform(double overlap_tshold, double ptmin=0.0);
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| 332 |
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| 333 |
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| 334 | //////////////////////////////
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| 335 | // save and debug functions //
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| 336 | //////////////////////////////
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| 337 |
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| 338 | /// save final jets
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| 339 | /// \param flux stream to save the jet contentss
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| 340 | int save_contents(FILE *flux);
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| 341 |
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| 342 | /// show jets/candidates status
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| 343 | int show();
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| 344 |
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| 345 | // particle information
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| 346 | int n; ///< number of particles
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| 347 | std::vector<Cmomentum> particles; ///< list of particles
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| 348 | std::vector<double> pt; ///< list of particles' pt
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| 349 | int n_left; ///< numer of particles that does not belong to any jet
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| 350 | std::vector<Cmomentum> p_remain; ///< list of particles remaining to deal with
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| 351 | std::vector<Cmomentum> p_uncol_hard; ///< list of particles remaining with collinear clustering
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| 352 | int n_pass; ///< index of the run
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| 353 |
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| 354 | /// minimal difference in squared distance between a particle and
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| 355 | /// two overlapping protojets when doing a split (useful when
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| 356 | /// testing approx. collinear safety)
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| 357 | double most_ambiguous_split;
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| 358 |
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| 359 | // jets information
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| 360 | std::vector<Cjet> jets; ///< list of jets
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| 361 |
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| 362 | // working entries
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| 363 | int *indices; ///< maximal size array for indices works
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| 364 | int idx_size; ///< number of elements in indices1
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| 365 |
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| 366 | /// The following flag indicates that identical protocones
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| 367 | /// are to be merged automatically each time around the split-merge
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| 368 | /// loop and before anything else happens.
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| 369 | ///
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| 370 | /// This flag is only effective if ALLOW_MERGE_IDENTICAL_PROTOCONES
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| 371 | /// is set in 'defines.h'
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| 372 | /// Note that this lead to infrared-unsafety so it is disabled
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| 373 | /// by default
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| 374 | bool merge_identical_protocones;
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| 375 |
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| 376 | /// member used for detailed comparisons of pt's
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| 377 | Csplit_merge_ptcomparison ptcomparison;
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| 378 |
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[273e668] | 379 | /// stop split--merge or progressive-removal when the squared SM_var
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| 380 | /// of the hardest protojet is below this cut-off. Note that this is
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| 381 | /// a signed square (ie SM_var*|SM_var|) to be able to handle
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| 382 | /// negative values.
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| 383 | ///
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[d7d2da3] | 384 | /// Note that the cut-off is set on the variable squared.
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| 385 | double SM_var2_hardest_cut_off;
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| 386 |
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| 387 | /// pt cutoff for the particles to put in p_uncol_hard
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| 388 | /// this is meant to allow removing soft particles in the
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| 389 | /// stable-cone search.
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[273e668] | 390 | ///
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| 391 | /// This is not collinear-safe so you should not use this
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| 392 | /// variable unless you really know what you are doing
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| 393 | /// Note that the cut-off is set on the variable squared.
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[d7d2da3] | 394 | double stable_cone_soft_pt2_cutoff;
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| 395 |
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| 396 | private:
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| 397 | /**
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| 398 | * get the overlap between 2 jets
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| 399 | * \param j1 first jet
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| 400 | * \param j2 second jet
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| 401 | * \param v returned overlap^2 (determined by the choice of SM variable)
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| 402 | * \return true if overlapping, false if disjoint
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| 403 | */
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| 404 | bool get_overlap(const Cjet &j1, const Cjet &j2, double *v);
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| 405 |
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| 406 |
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| 407 | /**
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| 408 | * split the two given jets.
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| 409 | * during this procedure, the jets j1 & j2 are replaced
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| 410 | * by 2 new jets. Common particles are associted to the
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| 411 | * closest initial jet.
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| 412 | * \param it_j1 iterator of the first jet in 'candidates'
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| 413 | * \param it_j2 iterator of the second jet in 'candidates'
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| 414 | * \param j1 first jet (Cjet instance)
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| 415 | * \param j2 second jet (Cjet instance)
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| 416 | * \return true on success, false on error
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| 417 | */
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| 418 | bool split(cjet_iterator &it_j1, cjet_iterator &it_j2);
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| 419 |
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| 420 | /**
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| 421 | * merge the two given jet.
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| 422 | * during this procedure, the jets j1 & j2 are replaced
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| 423 | * by 1 single jets containing both of them.
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| 424 | * \param it_j1 iterator of the first jet in 'candidates'
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| 425 | * \param it_j2 iterator of the second jet in 'candidates'
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| 426 | * \return true on success, false on error
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| 427 | */
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| 428 | bool merge(cjet_iterator &it_j1, cjet_iterator &it_j2);
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| 429 |
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| 430 | /**
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| 431 | * Check whether or not a jet has to be inserted in the
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| 432 | * list of protojets. If it has, set its sm_variable and
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| 433 | * insert it to the list of protojets.
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| 434 | * \param jet jet to insert
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| 435 | */
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| 436 | bool insert(Cjet &jet);
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| 437 |
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| 438 | /**
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| 439 | * given a 4-momentum and its associated pT, return the
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| 440 | * variable tht has to be used for SM
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| 441 | * \param v 4 momentum of the protojet
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| 442 | * \param pt_tilde pt_tilde of the protojet
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| 443 | */
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| 444 | double get_sm_var2(Cmomentum &v, double &pt_tilde);
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| 445 |
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| 446 | // jet information
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| 447 | /// list of jet candidates
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[969eb19] | 448 | #if __cplusplus < 201103L
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[d7d2da3] | 449 | std::auto_ptr<std::multiset<Cjet,Csplit_merge_ptcomparison> > candidates;
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[969eb19] | 450 | #else
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| 451 | std::unique_ptr<std::multiset<Cjet,Csplit_merge_ptcomparison> > candidates;
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[1d208a2] | 452 | #endif
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| 453 |
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[d7d2da3] | 454 | /// minimal pt2
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| 455 | double pt_min2;
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| 456 |
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| 457 | /**
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| 458 | * do we have or not to use the pt-weighted splitting
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| 459 | * (see description for set_pt_weighted_splitting)
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| 460 | * This will be false by default
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| 461 | */
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| 462 | bool use_pt_weighted_splitting;
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| 463 |
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[273e668] | 464 | /// use a user-defined scale to order the stable cones and jet
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| 465 | /// candidates
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| 466 | const Cuser_scale_base *_user_scale;
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| 467 |
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[d7d2da3] | 468 | #ifdef ALLOW_MERGE_IDENTICAL_PROTOCONES
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| 469 | /// checkxor for the candidates (to avoid having twice the same contents)
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| 470 | std::set<Creference> cand_refs;
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| 471 | #endif
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| 472 | };
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| 473 |
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| 474 | }
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| 475 |
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| 476 |
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| 477 | #endif
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