diff --git a/FixedOrderGen/include/PhaseSpacePoint.hh b/FixedOrderGen/include/PhaseSpacePoint.hh index 004c14d..ac8c452 100644 --- a/FixedOrderGen/include/PhaseSpacePoint.hh +++ b/FixedOrderGen/include/PhaseSpacePoint.hh @@ -1,199 +1,201 @@ /** \file PhaseSpacePoint.hh * \brief Contains the PhaseSpacePoint Class */ #pragma once #include #include "RHEJ/utility.hh" #include "RHEJ/Event.hh" #include "RHEJ/PDG_codes.hh" #include "RHEJ/PDF.hh" #include "RHEJ/RNG.hh" #include "Status.hh" #include "JetParameters.hh" #include "HiggsProperties.hh" namespace HEJFOG{ class Process; using RHEJ::Particle; //! A point in resummation phase space class PhaseSpacePoint{ public: //! Default PhaseSpacePoint Constructor PhaseSpacePoint() = default; //! PhaseSpacePoint Constructor /** * @param proc The process to generate * @param jet_def The Jet Definition Used * @param jetptmin Minimum Jet Transverse Momentum * @param rapmax Maximum parton rapidity * @param pdf The pdf set (used for sampling) * @param subl_chance Chance to turn a potentially subleading * emission (uno or central qqx) into an actual one * * Initially, only FKL phase space points are generated. subl_chance gives * the change of turning one emissions into a subleading configuration, * i.e. either unordered or central quark/anti-quark pair. Unordered * emissions require that the most extremal emission in any direction is * a quark or anti-quark and the next emission is a gluon. Quark/anti-quark * pairs are only generated for W processes. At most one subleading * emission will be generated in this way. */ PhaseSpacePoint( Process const & proc, JetParameters const & jet_properties, RHEJ::PDF & pdf, double E_beam, double subl_chance, HiggsProperties const & higgs_properties, RHEJ::RNG & ran ); //! Get Weight Function /** * @returns Weight of Event */ double weight() const{ return weight_; } Status status() const{ return status_; } //! Get Incoming Function /** * @returns Incoming Particles */ std::array const & incoming() const{ return incoming_; } //! Get Outgoing Function /** * @returns Outgoing Particles */ std::vector const & outgoing() const{ return outgoing_; } std::unordered_map> const & decays() const{ return decays_; } private: /** * \internal * \brief Generate LO parton momentum * * @param count Number of partons to generate * @param is_pure_jets If true ensures momentum conservation in x and y * @param jet_param Jet properties to fulfil * @param max_pt max allowed pt for a parton (typically E_CMS) * @param ran Random Number Generator * * @returns Momentum of partons * * Ensures that each parton is in its own jet. * Generation is independent of parton flavour. Output is sorted in rapidity. */ std::vector gen_LO_partons( int count, bool is_pure_jets, JetParameters const & jet_param, double max_pt, RHEJ::RNG & ran ); Particle gen_boson( RHEJ::ParticleID bosonid, double mass, double width, RHEJ::RNG & ran ); template fastjet::PseudoJet gen_last_momentum( ParticleMomenta const & other_momenta, double mass_square, double y ) const; bool jets_ok( std::vector const & Born_jets, std::vector const & partons ) const; /** * \internal * \brief Generate incoming partons according to the PDF * * @param uf Scale used in the PDF */ void reconstruct_incoming( Process const & proc, RHEJ::PDF & pdf, double E_beam, double uf, RHEJ::RNG & ran ); RHEJ::ParticleID generate_incoming_id( size_t beam_idx, double x, double uf, RHEJ::PDF & pdf, RHEJ::RNG & ran, bool allow_gluon=true ); bool momentum_conserved(double ep) const; RHEJ::Particle const & most_backward_FKL( std::vector const & partons ) const; RHEJ::Particle const & most_forward_FKL( std::vector const & partons ) const; RHEJ::Particle & most_backward_FKL(std::vector & partons) const; RHEJ::Particle & most_forward_FKL(std::vector & partons) const; bool extremal_FKL_ok( std::vector const & partons ) const; double random_normal(double stddev, RHEJ::RNG & ran); /** * @brief Turns a FKL configuration into a subleading one * * @param chance Change to switch to subleading configuration * @param proc Process to decide which subleading * configurations are allowed * * With a chance of "chance" the FKL configuration is either turned into * a unordered configuration or, for A/W/Z bosons, a configuration with * a central quark/anti-quark pair. */ void maybe_turn_to_subl(double chance, Process const & proc, RHEJ::RNG & ran); void turn_to_uno(bool can_be_uno_backward, bool can_be_uno_forward, RHEJ::RNG & ran); void turn_to_qqx(RHEJ::RNG & ran); std::vector decay_boson( RHEJ::Particle const & parent, std::vector const & decays, RHEJ::RNG & ran ); + /// @brief setup outgoing partons to ensure correct coupling to boson + void couple_boson(RHEJ::ParticleID boson, RHEJ::RNG & ran); Decay select_decay_channel( std::vector const & decays, RHEJ::RNG & ran ); double gen_hard_pt( int np, double ptmin, double ptmax, double y, RHEJ::RNG & ran ); double gen_soft_pt(int np, double ptmax, RHEJ::RNG & ran); double gen_parton_pt( int count, JetParameters const & jet_param, double ptmax, double y, RHEJ::RNG & ran ); double weight_; Status status_; std::array incoming_; std::vector outgoing_; //! Particle decays in the format {outgoing index, decay products} std::unordered_map> decays_; }; RHEJ::UnclusteredEvent to_UnclusteredEvent(PhaseSpacePoint const & psp); } diff --git a/FixedOrderGen/include/Status.hh b/FixedOrderGen/include/Status.hh index 54fdc0b..88d2155 100644 --- a/FixedOrderGen/include/Status.hh +++ b/FixedOrderGen/include/Status.hh @@ -1,22 +1,24 @@ #pragma once #include #include namespace HEJFOG{ enum Status{ good, not_enough_jets, - too_much_energy + too_much_energy, + wrong_final_state /// @TODO remove this state }; inline std::string to_string(Status s){ switch(s){ - case good: return "good"; - case not_enough_jets: return "not enough jets"; - case too_much_energy: return "too much energy"; - default:; + case good: return "good"; + case not_enough_jets: return "not enough jets"; + case too_much_energy: return "too much energy"; + case wrong_final_state: return "wrong final state"; + default:; } throw std::logic_error{"unreachable"}; } } diff --git a/FixedOrderGen/src/PhaseSpacePoint.cc b/FixedOrderGen/src/PhaseSpacePoint.cc index 2432400..abbc20a 100644 --- a/FixedOrderGen/src/PhaseSpacePoint.cc +++ b/FixedOrderGen/src/PhaseSpacePoint.cc @@ -1,613 +1,656 @@ #include "PhaseSpacePoint.hh" #include #include #include "RHEJ/Constants.hh" #include "RHEJ/kinematics.hh" #include "RHEJ/utility.hh" #include "RHEJ/exceptions.hh" #include "Process.hh" #include #include using namespace RHEJ; namespace HEJFOG{ static_assert( std::numeric_limits::has_quiet_NaN, "no quiet NaN for double" ); constexpr double NaN = std::numeric_limits::quiet_NaN(); RHEJ::UnclusteredEvent to_UnclusteredEvent(PhaseSpacePoint const & psp){ RHEJ::UnclusteredEvent result; result.incoming = psp.incoming(); std::sort( begin(result.incoming), end(result.incoming), [](Particle o1, Particle o2){return o1.p.pz()= 2); result.decays = psp.decays(); result.central.mur = NaN; result.central.muf = NaN; result.central.weight = psp.weight(); return result; } namespace{ bool can_swap_to_uno( RHEJ::Particle const & p1, RHEJ::Particle const & p2 ){ return is_parton(p1) && p1.type != pid::gluon && p2.type == pid::gluon; } size_t count_gluons(std::vector::const_iterator first, std::vector::const_iterator last){ return std::count_if(first, last, [](Particle const & p) {return p.type == pid::gluon;}); } /** assumes FKL configurations between first and last, * else there can be a quark in a non-extreme position * e.g. uno configuration gqg would pass */ bool can_change_to_qqx( std::vector::const_iterator first, std::vector::const_iterator last){ return 1 < count_gluons(first,last); } bool is_AWZ_proccess(Process const & proc){ return proc.boson && is_AWZ_boson(*proc.boson); } } void PhaseSpacePoint::maybe_turn_to_subl( double chance, Process const & proc, RHEJ::RNG & ran ){ if(proc.njets <= 2) return; assert(outgoing_.size() >= 2); // decide what kind of subleading process is allowed bool allow_uno = false; const size_t nout = outgoing_.size(); const bool can_be_uno_backward = can_swap_to_uno( outgoing_[0], outgoing_[1] ); const bool can_be_uno_forward = can_swap_to_uno( outgoing_[nout-1], outgoing_[nout-2] ); allow_uno = can_be_uno_backward || can_be_uno_forward; bool allow_qqx = false; if(is_AWZ_proccess(proc)) { allow_qqx = can_change_to_qqx(outgoing_.cbegin(), outgoing_.cend()); if(incoming_[0].type == pid::gluon && incoming_[1].type == pid::gluon) { /// enforce qqx for initial gg allow_uno = false; chance = 1.; } } if(!allow_uno && !allow_qqx) return; if(ran.flat() < chance){ weight_ /= chance; if(allow_uno && !allow_qqx){ turn_to_uno(can_be_uno_backward, can_be_uno_forward, ran); } else if (!allow_uno && allow_qqx) { std::cout << "only qqx" << std::endl; turn_to_qqx(ran); } else { assert( allow_uno && allow_qqx); std::cout << "both qqx and uno" << std::endl; if(ran.flat() < 0.5) turn_to_uno(can_be_uno_backward, can_be_uno_forward, ran); else turn_to_qqx(ran); weight_ *= 2.; } } else weight_ /= 1 - chance; } void PhaseSpacePoint::turn_to_uno( const bool can_be_uno_backward, const bool can_be_uno_forward, RHEJ::RNG & ran ){ if(!can_be_uno_backward && !can_be_uno_forward) return; const size_t nout = outgoing_.size(); if(can_be_uno_backward && can_be_uno_forward){ if(ran.flat() < 0.5){ std::swap(outgoing_[0].type, outgoing_[1].type); } else { std::swap(outgoing_[nout-1].type, outgoing_[nout-2].type); } weight_ *= 2.; } else if(can_be_uno_backward){ std::swap(outgoing_[0].type, outgoing_[1].type); } else { assert(can_be_uno_forward); std::swap(outgoing_[nout-1].type, outgoing_[nout-2].type); } } void PhaseSpacePoint::turn_to_qqx(RHEJ::RNG & ran){ /// find first and last gluon in FKL chain auto first = std::find_if(outgoing_.begin(), outgoing_.end(), [](Particle const & p){return p.type == pid::gluon;}); auto last = std::find_if(first, outgoing_.end(), [](Particle const & p){return is_quark(p) || is_antiquark(p);}); const size_t ng = count_gluons(first,last); if(ng < 2) throw std::logic_error("not enough gluons to create qqx"); // select flavour of quark const double r1 = 2.*ran.flat()-1.; weight_ *= n_f*2; int flavour = pid::down; for (double sum = 1./n_f; sum < std::abs(r1); sum += 1./n_f) ++flavour; flavour*=r1<0.?-1:1; // select gluon for switch first += floor((ng-1) * ran.flat()); auto next = std::find_if(first+1, last, [](Particle const & p){return p.type == pid::gluon;}); assert(next != outgoing_.end()); weight_ *= (ng-1); first->type = ParticleID(flavour); next->type = ParticleID(-flavour); } template fastjet::PseudoJet PhaseSpacePoint::gen_last_momentum( ParticleMomenta const & other_momenta, const double mass_square, const double y ) const { std::array pt{0.,0.}; for (auto const & p: other_momenta) { pt[0]-= p.px(); pt[1]-= p.py(); } const double mperp = sqrt(pt[0]*pt[0]+pt[1]*pt[1]+mass_square); const double pz=mperp*sinh(y); const double E=mperp*cosh(y); return {pt[0], pt[1], pz, E}; } PhaseSpacePoint::PhaseSpacePoint( Process const & proc, JetParameters const & jet_param, RHEJ::PDF & pdf, double E_beam, double subl_chance, HiggsProperties const & h, RHEJ::RNG & ran ) { assert(proc.njets >= 2); status_ = good; weight_ = 1; const int nout = proc.njets + (proc.boson?1:0); outgoing_.reserve(nout); // generate parton momenta const bool is_pure_jets = !proc.boson; auto partons = gen_LO_partons( proc.njets, is_pure_jets, jet_param, E_beam, ran ); // pre fill flavour with gluons for(auto&& p_out: partons) { outgoing_.emplace_back(Particle{pid::gluon, std::move(p_out)}); } if(status_ != good) return; if(proc.boson){ switch (*proc.boson) { case pid::Higgs:{ auto Hparticle=gen_boson(pid::higgs, h.mass, h.width, ran); auto pos=std::upper_bound( begin(outgoing_),end(outgoing_),Hparticle,rapidity_less{} ); outgoing_.insert(pos, Hparticle); if(! h.decays.empty()){ const int boson_idx = std::distance(begin(outgoing_), pos); decays_.emplace( boson_idx, decay_boson(outgoing_[boson_idx], h.decays, ran) ); } break; } case pid::Wp:{ /// @TODO implement, currently this is just a relabel Higgs ///@{ std::cout << "Emission of Wp not implemented yet.\nThis is just a place holder" << std::endl; auto Hparticle=gen_boson(pid::Wp, h.mass, h.width, ran); auto pos=std::upper_bound( begin(outgoing_),end(outgoing_),Hparticle,rapidity_less{} ); outgoing_.insert(pos, Hparticle); if(! h.decays.empty()){ const int boson_idx = std::distance(begin(outgoing_), pos); decays_.emplace( boson_idx, decay_boson(outgoing_[boson_idx], h.decays, ran) ); } ///@} break; } case pid::Wm:{ /// @TODO implement, currently this is just a relabel Higgs ///@{ std::cout << "Emission of Wm not implemented yet.\nThis is just a place holder" << std::endl; auto Hparticle=gen_boson(pid::higgs, h.mass, h.width, ran); auto pos=std::upper_bound( begin(outgoing_),end(outgoing_),Hparticle,rapidity_less{} ); outgoing_.insert(pos, Hparticle); if(! h.decays.empty()){ const int boson_idx = std::distance(begin(outgoing_), pos); decays_.emplace( boson_idx, decay_boson(outgoing_[boson_idx], h.decays, ran) ); } ///@} break; } case pid::photon: case pid::Z: default: throw std::logic_error("Emission of boson of unsupported type"); } } // normalisation of momentum-conserving delta function weight_ *= pow(2*M_PI, 4); reconstruct_incoming(proc, pdf, E_beam, jet_param.min_pt, ran); if(status_ != good) return; // set outgoing states most_backward_FKL(outgoing_).type = incoming_[0].type; most_forward_FKL(outgoing_).type = incoming_[1].type; maybe_turn_to_subl(subl_chance, proc, ran); + if(proc.boson) couple_boson(*proc.boson, ran); + #ifndef NDEBUG if(is_AWZ_proccess(proc)){ // check that W has a quark to couple to auto const partons = filter_partons(outgoing_); /// @TODO extend assert to also check flavour? Maybe easier in separate cmake test assert(partons.front().type != pid::gluon || partons.back().type != pid::gluon // extremal quark || ( (partons.size() > 3 ) // or central qqx && ( 1 p_small_pt) { weight_ /= 1. - p_small_pt; return gen_hard_pt(count, *jet_param.peak_pt, max_pt, y, ran); } weight_ /= p_small_pt; const double pt = gen_soft_pt(count, *jet_param.peak_pt, ran); if(pt < jet_param.min_pt) { weight_=0.0; status_ = not_enough_jets; return jet_param.min_pt; } return pt; } std::vector PhaseSpacePoint::gen_LO_partons( int np, bool is_pure_jets, JetParameters const & jet_param, double max_pt, RHEJ::RNG & ran ){ if (np<2) throw std::invalid_argument{"Not enough partons in gen_LO_partons"}; weight_ /= pow(16.*pow(M_PI,3),np); weight_ /= std::tgamma(np+1); //remove rapidity ordering std::vector partons; partons.reserve(np); for(int i = 0; i < np; ++i){ const double y = -jet_param.max_y + 2*jet_param.max_y*ran.flat(); weight_ *= 2*jet_param.max_y; const bool is_last_parton = i+1 == np; if(is_pure_jets && is_last_parton) { constexpr double parton_mass_sq = 0.; partons.emplace_back(gen_last_momentum(partons, parton_mass_sq, y)); break; } const double phi = 2*M_PI*ran.flat(); weight_ *= 2.0*M_PI; const double pt = gen_parton_pt(np, jet_param, max_pt, y, ran); if(weight_ == 0.0) return {}; partons.emplace_back(fastjet::PtYPhiM(pt, y, phi)); assert(jet_param.min_pt <= partons[i].pt()); assert(partons[i].pt() <= max_pt+1e-5); } // Need to check that at LO, the number of jets = number of partons; fastjet::ClusterSequence cs(partons, jet_param.def); auto cluster_jets=cs.inclusive_jets(jet_param.min_pt); if (cluster_jets.size()!=unsigned(np)){ weight_=0.0; status_ = not_enough_jets; return {}; } std::sort(begin(partons), end(partons), rapidity_less{}); return partons; } Particle PhaseSpacePoint::gen_boson( RHEJ::ParticleID bosonid, double mass, double width, RHEJ::RNG & ran ){ // Usual phase space measure weight_ /= 16.*pow(M_PI, 3); // Generate a y Gaussian distributed around 0 // TODO: magic number only for Higgs const double y = random_normal(1.6, ran); const double r1 = ran.flat(); const double sH = mass*( mass + width*tan(M_PI/2.*r1 + (r1-1.)*atan(mass/width)) ); auto p = gen_last_momentum(outgoing_, sH, y); return Particle{bosonid, std::move(p)}; } Particle const & PhaseSpacePoint::most_backward_FKL( std::vector const & partons ) const{ if(!RHEJ::is_parton(partons[0])) return partons[1]; return partons[0]; } Particle const & PhaseSpacePoint::most_forward_FKL( std::vector const & partons ) const{ const size_t last_idx = partons.size() - 1; if(!RHEJ::is_parton(partons[last_idx])) return partons[last_idx-1]; return partons[last_idx]; } Particle & PhaseSpacePoint::most_backward_FKL( std::vector & partons ) const{ if(!RHEJ::is_parton(partons[0])) return partons[1]; return partons[0]; } Particle & PhaseSpacePoint::most_forward_FKL( std::vector & partons ) const{ const size_t last_idx = partons.size() - 1; if(!RHEJ::is_parton(partons[last_idx])) return partons[last_idx-1]; return partons[last_idx]; } void PhaseSpacePoint::reconstruct_incoming( Process const & proc, RHEJ::PDF & pdf, double E_beam, double uf, RHEJ::RNG & ran ){ std::tie(incoming_[0].p, incoming_[1].p) = incoming_momenta(outgoing_); // calculate xa, xb const double sqrts=2*E_beam; const double xa=(incoming_[0].p.e()-incoming_[0].p.pz())/sqrts; const double xb=(incoming_[1].p.e()+incoming_[1].p.pz())/sqrts; // abort if phase space point is outside of collider energy reach if (xa>1. || xb>1.){ weight_=0; status_ = too_much_energy; return; } // pick pdfs /** @TODO * ufa, ufb don't correspond to our final scale choice. * The reversed HEJ scale generators currently expect a full event as input, * so fixing this is not completely trivial */ auto const & ids = proc.incoming; bool allow_gluon = 1; // special case W2j: needs one quark initially if(proc.njets == 2 && is_AWZ_proccess(proc)){ + // @TODO optimise: do not allow dd initial for Wp, also for 3j if(ids[0] == pid::gluon || ids[1] == pid::gluon){ // one gluon -> other has to be quark allow_gluon = 0; if(ids[0] == ids[1]){ // both gluons throw RHEJ::not_implemented{ "W+2 jet process requires at least one initial quark" }; } } else { // else force one to be a gluon allow_gluon = ran.flat() < 0.5; // @TODO better sample weight_*=2.; } } for(size_t i = 0; i < 2; ++i){ if(ids[i] == pid::proton || ids[i] == pid::p_bar){ incoming_[i].type = generate_incoming_id(i, i?xb:xa, uf, pdf, ran, allow_gluon); if(allow_gluon && proc.njets == 2 && is_AWZ_proccess(proc)) allow_gluon = 0; // no gluon in first -> must be second } else { incoming_[i].type = ids[i]; } } assert(momentum_conserved(1e-7)); } namespace { /// particles are ordered, odd = anti ParticleID index_to_pid(size_t i){ if(!i) return pid::gluon; return static_cast(i%2?(i+1)/2:-i/2); } } RHEJ::ParticleID PhaseSpacePoint::generate_incoming_id( size_t const beam_idx, double const x, double const uf, RHEJ::PDF & pdf, RHEJ::RNG & ran, bool allow_gluon ){ std::array pdf_wt; pdf_wt[0] = allow_gluon?fabs(pdf.pdfpt(beam_idx,x,uf,pid::gluon)):0.; double pdftot = pdf_wt[0]; for(size_t i = 1; i < pdf_wt.size(); ++i){ pdf_wt[i] = 4./9.*fabs(pdf.pdfpt(beam_idx,x,uf,index_to_pid(i))); pdftot += pdf_wt[i]; } const double r1 = pdftot * ran.flat(); double sum = 0; for(size_t i=0; i < pdf_wt.size(); ++i){ if (r1 < (sum+=pdf_wt[i])){ weight_*= pdftot/pdf_wt[i]; return index_to_pid(i); } } std::cerr << "Error in choosing incoming parton: "<0?1:-1; + std::vector allowed_parts; + for(auto & part: outgoing_){ + // Wp -> up OR anti-down, Wm -> anti-up OR down + if ( (sign_W*part.type > 0 && is_up_type(part)) + || (sign_W*part.type < 0 && is_down_type(part)) ) + allowed_parts.push_back(&part); + } + if(!allowed_parts.size()){ + /// @TODO do not allow such states in the generation + status_=wrong_final_state; + return; + } + + // select one and flip it + size_t idx = 0; + if(allowed_parts.size() > 1){ + /// @TODO more efficient sampling + idx = floor(ran.flat()*allowed_parts.size()); + weight_ *= allowed_parts.size(); + } + allowed_parts[idx]->type = + static_cast( allowed_parts[idx]->type - sign_W ); + } + double PhaseSpacePoint::random_normal( double stddev, RHEJ::RNG & ran ){ const double r1 = ran.flat(); const double r2 = ran.flat(); const double lninvr1 = -log(r1); const double result = stddev*sqrt(2.*lninvr1)*cos(2.*M_PI*r2); weight_ *= exp(result*result/(2*stddev*stddev))*sqrt(2.*M_PI)*stddev; return result; } bool PhaseSpacePoint::momentum_conserved(double ep) const{ fastjet::PseudoJet diff; for(auto const & in: incoming()) diff += in.p; for(auto const & out: outgoing()) diff -= out.p; return nearby_ep(diff, fastjet::PseudoJet{}, ep); } Decay PhaseSpacePoint::select_decay_channel( std::vector const & decays, RHEJ::RNG & ran ){ double br_total = 0.; for(auto const & decay: decays) br_total += decay.branching_ratio; // adjust weight // this is given by (channel branching ratio)/(chance to pick channel) // where (chance to pick channel) = // (channel branching ratio)/(total branching ratio) weight_ *= br_total; const double r1 = br_total*ran.flat(); double br_sum = 0.; for(auto const & decay: decays){ br_sum += decay.branching_ratio; if(r1 < br_sum) return decay; } throw std::logic_error{"unreachable"}; } std::vector PhaseSpacePoint::decay_boson( RHEJ::Particle const & parent, std::vector const & decays, RHEJ::RNG & ran ){ const auto channel = select_decay_channel(decays, ran); if(channel.products.size() != 2){ throw RHEJ::not_implemented{ "only decays into two particles are implemented" }; } std::vector decay_products(channel.products.size()); for(size_t i = 0; i < channel.products.size(); ++i){ decay_products[i].type = channel.products[i]; } // choose polar and azimuth angle in parent rest frame const double E = parent.m()/2; const double theta = 2.*M_PI*ran.flat(); const double cos_phi = 2.*ran.flat()-1.; const double sin_phi = sqrt(1. - cos_phi*cos_phi); // Know 0 < phi < pi const double px = E*cos(theta)*sin_phi; const double py = E*sin(theta)*sin_phi; const double pz = E*cos_phi; decay_products[0].p.reset(px, py, pz, E); decay_products[1].p.reset(-px, -py, -pz, E); for(auto & particle: decay_products) particle.p.boost(parent.p); return decay_products; } }