// -*- C++ -*- /////////////////////////////////////////////////////////////////////////////// // File: split_merge.h // // Description: header file for splitting/merging (contains the CJet class) // // This file is part of the SISCone project. // // For more details, see http://projects.hepforge.org/siscone // // // // Copyright (c) 2006 Gavin Salam and Gregory Soyez // // // // This program is free software; you can redistribute it and/or modify // // it under the terms of the GNU General Public License as published by // // the Free Software Foundation; either version 2 of the License, or // // (at your option) any later version. // // // // This program is distributed in the hope that it will be useful, // // but WITHOUT ANY WARRANTY; without even the implied warranty of // // MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the // // GNU General Public License for more details. // // // // You should have received a copy of the GNU General Public License // // along with this program; if not, write to the Free Software // // Foundation, Inc., 51 Franklin St, Fifth Floor, Boston, MA 02110-1301, USA // // // // $Revision: 1.1 $// // $Date: 2008-10-02 15:20:30 $// /////////////////////////////////////////////////////////////////////////////// #ifndef __SPLIT_MERGE_H__ #define __SPLIT_MERGE_H__ #include "defines.h" #include "geom_2d.h" #include "momentum.h" #include #include #include #include #include namespace siscone{ /** * \class Cjet * real Jet information. * * This class contains information for one single jet. * That is, first, its momentum carrying information * about its centre and pT, and second, its particle * contents */ class Cjet{ public: /// default ctor Cjet(); /// default dtor ~Cjet(); Cmomentum v; ///< jet momentum double pt_tilde; ///< p-scheme pt int n; ///< number of particles inside std::vector contents; ///< particle contents (list of indices) /// ordering variable used for ordering and overlap in the /// split--merge. This variable is automatically set either to /// pt_tilde, or to mt or to pt, depending on the siscone /// parameter. Note that the default behaviour is pt_tilde and that /// other chices may lead to infrared unsafe situations. /// Note: we use the square of the varible rather than the variable itself double sm_var2; /// covered range in eta-phi Ceta_phi_range range; /// pass at which the jet has been found /// It starts at 0 (first pass), -1 means infinite rapidity int pass; }; /// ordering of jets in pt (e.g. used in final jets ordering) bool jets_pt_less(const Cjet &j1, const Cjet &j2); /// the choices of scale variable that can be used in the split-merge /// step, both for ordering the protojets and for measuing their /// overlap; pt, Et and mt=sqrt(pt^2+m^2) are all defined in E-scheme /// (4-momentum) recombination; pttilde = \sum_{i\in jet} |p_{t,i}| /// /// NB: if one changes the order here, one _MUST_ also change the order /// in the SISCone plugin enum Esplit_merge_scale { SM_pt, ///< transverse momentum (E-scheme), IR unsafe SM_Et, ///< transverse energy (E-scheme), not long. boost inv. ///< original run-II choice [may not be implemented] SM_mt, ///< transverse mass (E-scheme), IR safe except ///< in decays of two identical narrow heavy particles SM_pttilde ///< pt-scheme pt = \sum_{i in jet} |p_{ti}|, should ///< be IR safe in all cases }; /// return the name of the split-merge scale choice std::string split_merge_scale_name(Esplit_merge_scale sms); /** * \class Csplit_merge_comparison * a class that allows us to carry out comparisons of pt of jets, using * information from exact particle contents where necessary. * */ class Csplit_merge_ptcomparison{ public: Csplit_merge_ptcomparison() : particles(0), split_merge_scale(SM_pttilde){}; // return the name corresponding to the SM scale variable std::string SM_scale_name() const { return split_merge_scale_name(split_merge_scale);} std::vector * particles; std::vector * pt; bool operator()(const Cjet &jet1, const Cjet &jet2) const; /** * get the difference between 2 jets, calculated such that rounding * errors will not affect the result even if the two jets have * almost the same content (so that the difference is below the * rounding errors) * * \param j1 first jet * \param j2 second jet * \param v jet1-jet2 * \param pt_tilde jet1-jet2 pt_tilde */ void get_difference(const Cjet &j1, const Cjet &j2, Cmomentum *v, double *pt_tilde) const; /// the following parameter controls the variable we're using for /// the split-merge process i.e. the variable we use for /// 1. ordering jet candidates; /// 2. computing te overlap fraction of two candidates. /// The default value uses pttile (p-scheme pt). Other alternatives are /// pt, mt=sqrt(pt^2+m^2)=sqrt(E^2-pz^2) or Et. /// NOTE: Modifying the default choice can have nasty effects: /// - using pt leads to some IR unsafety when we have two jets, /// e.g. back-to-back, with the same pt. In that case, their ordering /// in pt is random and can be affected by the addition of a /// soft particle. Hence, we highly recommand to keep this to /// the default value i.e. to use pt only for the purpose of /// investigating the IR issue /// - using Et is safe but do not respect boost invariance /// - using mt solves the IR unsafety issues with the pt variable /// for QCD jets but the IR unsafety remains for nack-to-back /// jets of unstable narrow-width particles (e.g. Higgs). /// Therefore, keeping the default value is strongly advised. Esplit_merge_scale split_merge_scale; }; // iterator types /// iterator definition for the jet candidates structure typedef std::multiset::iterator cjet_iterator; /// iterator definition for the jet structure typedef std::vector::iterator jet_iterator; /** * \class Csplit_merge * Class used to split and merge jets. */ class Csplit_merge{ public: /// default ctor Csplit_merge(); /// default dtor ~Csplit_merge(); ////////////////////////////// // initialisation functions // ////////////////////////////// /** * initialisation function * \param _particles list of particles * \param protocones list of protocones (initial jet candidates) * \param R2 cone radius (squared) * \param ptmin minimal pT allowed for jets * \return 0 on success, 1 on error */ int init(std::vector &_particles, std::vector *protocones, double R2, double ptmin=0.0); /** * initialisation function for particle list * \param _particles list of particles * \return 0 on success, 1 on error */ int init_particles(std::vector &_particles); /** * build initial list of left particles */ int init_pleft(); //////////////////////// // cleaning functions // //////////////////////// /// partial clearance int partial_clear(); /// full clearance int full_clear(); ///////////////////////////////// // main parts of the algorithm // ///////////////////////////////// /** * build the list 'p_uncol_hard' from p_remain by clustering * collinear particles and removing particles softer than * stable_cone_soft_pt2_cutoff * note that thins in only used for stable-cone detection * so the parent_index field is unnecessary */ int merge_collinear_and_remove_soft(); /** * add a list of protocones * \param protocones list of protocones (initial jet candidates) * \param R2 cone radius (squared) * \param ptmin minimal pT allowed for jets * \return 0 on success, 1 on error */ int add_protocones(std::vector *protocones, double R2, double ptmin=0.0); /** * really do the splitting and merging * At the end, the vector jets is filled with the jets found. * the 'contents' field of each jets contains the indices * of the particles included in that jet. * \param overlap_tshold threshold for splitting/merging transition * \param ptmin minimal pT allowed for jets * \return the number of jets is returned */ int perform(double overlap_tshold, double ptmin=0.0); ////////////////////////////// // save and debug functions // ////////////////////////////// /// save final jets /// \param flux stream to save the jet contentss int save_contents(FILE *flux); /// show jets/candidates status int show(); // particle information int n; ///< number of particles std::vector particles; ///< list of particles std::vector pt; ///< list of particles' pt int n_left; ///< numer of particles that does not belong to any jet std::vector p_remain; ///< list of particles remaining to deal with std::vector p_uncol_hard; ///< list of particles remaining with collinear clustering int n_pass; ///< index of the run /// minimal difference in squared distance between a particle and /// two overlapping protojets when doing a split (useful when /// testing approx. collinear safety) double most_ambiguous_split; // jets information std::vector jets; ///< list of jets // working entries int *indices; ///< maximal size array for indices works int idx_size; ///< number of elements in indices1 /// The following flag indicates that identical protocones /// are to be merged automatically each time around the split-merge /// loop and before anything else happens. /// /// This flag is only effective if ALLOW_MERGE_IDENTICAL_PROTOCONES /// is set in 'defines.h' /// Note that this lead to infrared-unsafety so it is disabled /// by default bool merge_identical_protocones; /// member used for detailed comparisons of pt's Csplit_merge_ptcomparison ptcomparison; /// stop split--merge when the SM_var of the hardest protojet /// is below this cut-off. /// This is not collinear-safe so you should not use this /// variable unless you really know what you are doing /// Note that the cut-off is set on the variable squared. double SM_var2_hardest_cut_off; /// pt cutoff for the particles to put in p_uncol_hard /// this is meant to allow removing soft particles in the /// stable-cone search. double stable_cone_soft_pt2_cutoff; private: /** * get the overlap between 2 jets * \param j1 first jet * \param j2 second jet * \param v returned overlap^2 (determined by the choice of SM variable) * \return true if overlapping, false if disjoint */ bool get_overlap(const Cjet &j1, const Cjet &j2, double *v); /** * split the two given jets. * during this procedure, the jets j1 & j2 are replaced * by 2 new jets. Common particles are associted to the * closest initial jet. * \param it_j1 iterator of the first jet in 'candidates' * \param it_j2 iterator of the second jet in 'candidates' * \param j1 first jet (Cjet instance) * \param j2 second jet (Cjet instance) * \return true on success, false on error */ bool split(cjet_iterator &it_j1, cjet_iterator &it_j2); /** * merge the two given jet. * during this procedure, the jets j1 & j2 are replaced * by 1 single jets containing both of them. * \param it_j1 iterator of the first jet in 'candidates' * \param it_j2 iterator of the second jet in 'candidates' * \return true on success, false on error */ bool merge(cjet_iterator &it_j1, cjet_iterator &it_j2); /** * Check whether or not a jet has to be inserted in the * list of protojets. If it has, set its sm_variable and * insert it to the list of protojets. * \param jet jet to insert */ bool insert(Cjet &jet); /** * given a 4-momentum and its associated pT, return the * variable tht has to be used for SM * \param v 4 momentum of the protojet * \param pt_tilde pt_tilde of the protojet */ double get_sm_var2(Cmomentum &v, double &pt_tilde); // jet information /// list of jet candidates std::auto_ptr > candidates; /// minimal pt2 double pt_min2; #ifdef ALLOW_MERGE_IDENTICAL_PROTOCONES /// checkxor for the candidates (to avoid having twice the same contents) std::set cand_refs; #endif }; } #endif