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 // PowhegHooks.h is a part of the PYTHIA event generator.
 // Copyright (C) 2025 Richard Corke, Torbjorn Sjostrand.
 // PYTHIA is licenced under the GNU GPL v2 or later, see COPYING for details.
 // Please respect the MCnet Guidelines, see GUIDELINES for details.
 
 // Author: Richard Corke, modified by Christian T Preuss.
 // This class is used to perform a vetoed shower, where emissions
 // already covered in a POWHEG NLO generator should be omitted.
 // To first approximation the handover should happen at the SCALE
 // of the LHA, but since the POWHEG-BOX uses a different pT definition
 // than PYTHIA, both for ISR and FSR, a more sophisticated treatment
 // is needed. See the online manual on POWHEG matching for details.
 
 #ifndef Pythia8_PowhegHooks_H
 #define Pythia8_PowhegHooks_H
 
 // Includes
 #include "Pythia8/Pythia.h"
 #include "Pythia8/Plugins.h"
 
 namespace Pythia8 {
 
 //==========================================================================
 
 // Use userhooks to veto PYTHIA emissions above the POWHEG scale.
 
 class PowhegHooks : public UserHooks {
 
 public:
 
   // Constructors and destructor.
   PowhegHooks() {}
   PowhegHooks(Pythia*, Settings*, Logger*) {}
   ~PowhegHooks() {}
 
   //--------------------------------------------------------------------------
 
   // Initialize settings, detailing merging strategy to use.
   bool initAfterBeams() {
     nFinal      = settingsPtr->mode("POWHEG:nFinal");
     vetoMode    = settingsPtr->mode("POWHEG:veto");
     vetoCount   = settingsPtr->mode("POWHEG:vetoCount");
     pThardMode  = settingsPtr->mode("POWHEG:pThard");
     pTemtMode   = settingsPtr->mode("POWHEG:pTemt");
     emittedMode = settingsPtr->mode("POWHEG:emitted");
     pTdefMode   = settingsPtr->mode("POWHEG:pTdef");
     MPIvetoMode = settingsPtr->mode("POWHEG:MPIveto");
     QEDvetoMode = settingsPtr->mode("POWHEG:QEDveto");
     showerModel = settingsPtr->mode("PartonShowers:model");
     return true;
   }
 
   //--------------------------------------------------------------------------
 
   // Routines to calculate the pT (according to pTdefMode) in a branching:
   //   ISR: i (radiator after)  -> j (emitted after) k (radiator before)
   //   FSR: i (radiator before) -> j (emitted after) k (radiator after)
   // For the Pythia pT definitions, a recoiler (after) must be specified.
 
   // Top-level wrapper for shower pTs.
   inline double pT(const Event& e, int RadAfterBranch,
     int EmtAfterBranch, int RecAfterBranch, bool FSR) {
     // VINCIA pT definition.
     if (showerModel == 2)
       return pTvincia(e, RadAfterBranch, EmtAfterBranch, RecAfterBranch);
     // Simple-shower pT definition.
     return pTpythia(e, RadAfterBranch, EmtAfterBranch, RecAfterBranch, FSR);
   }
 
   //--------------------------------------------------------------------------
 
   // Compute the Pythia pT separation.
   // Based on pTLund function in History.cc and identical to pTevol.
   inline double pTpythia(const Event& e, int RadAfterBranch,
     int EmtAfterBranch, int RecAfterBranch, bool FSR) {
 
     // Convenient shorthands for later
     Vec4 radVec = e[RadAfterBranch].p();
     Vec4 emtVec = e[EmtAfterBranch].p();
     Vec4 recVec = e[RecAfterBranch].p();
     int  radID  = e[RadAfterBranch].id();
 
     // Calculate virtuality of splitting
     double sign = (FSR) ? 1. : -1.;
     Vec4 Q(radVec + sign * emtVec);
     double Qsq = sign * Q.m2Calc();
 
     // Mass term of radiator
     double m2Rad = (abs(radID) >= 4 && abs(radID) < 7) ?
                    pow2(particleDataPtr->m0(radID)) : 0.;
 
     // z values for FSR and ISR
     double z, pTnow;
     if (FSR) {
       // Construct 2 -> 3 variables
       Vec4 sum = radVec + recVec + emtVec;
       double m2Dip = sum.m2Calc();
       double x1 = 2. * (sum * radVec) / m2Dip;
       double x3 = 2. * (sum * emtVec) / m2Dip;
       z     = x1 / (x1 + x3);
       pTnow = z * (1. - z);
 
     } else {
       // Construct dipoles before/after splitting
       Vec4 qBR(radVec - emtVec + recVec);
       Vec4 qAR(radVec + recVec);
       z     = qBR.m2Calc() / qAR.m2Calc();
       pTnow = (1. - z);
     }
 
     // Virtuality with correct sign
     pTnow *= (Qsq - sign * m2Rad);
 
     // Can get negative pT for massive splittings.
     if (pTnow < 0.) {
       loggerPtr->WARNING_MSG("negative pT");
       return -1.;
     }
 
     // Return pT
     return sqrt(pTnow);
   }
 
   //--------------------------------------------------------------------------
 
   // Compute the Vincia pT as in Eq. (2.63)-(2.66) in arXiv:2003.00702.
   // Branching is assumed to be {13} {23} -> 1 3 2.
   inline double pTvincia(const Event& event, int i1, int i3, int i2) {
 
     // Shorthands.
     Vec4 p1 = event[i1].p();
     Vec4 p3 = event[i3].p();
     Vec4 p2 = event[i2].p();
 
     // Fetch mothers of 1 and 2.
     int iMoth1 = event[i1].mother1();
     int iMoth2 = event[i2].mother1();
     if (iMoth1 == 0 || iMoth2 == 0) {
       loggerPtr->ABORT_MSG("could not find mothers of particles");
       exit(1);
     }
 
     // Invariants defined as in Eq. (5) in arXiv:2008.09468.
     double mMoth1Sq = event[iMoth1].m2();
     double mMoth2Sq = event[iMoth2].m2();
     double sgn1 = event[i1].isFinal() ? 1. : -1.;
     double sgn2 = event[i2].isFinal() ? 1. : -1.;
     double qSq13 = sgn1*(m2(sgn1*p1+p3) - mMoth1Sq);
     double qSq23 = sgn2*(m2(sgn2*p2+p3) - mMoth2Sq);
 
     // Normalisation as in Eq. (6) in arXiv:2008.09468.
     double sMax = -1.;
     if (event[i1].isFinal() && event[i2].isFinal()) {
       // FF.
       sMax = m2(p1+p2+p3) - mMoth1Sq - mMoth2Sq;
     } else if ((event[i1].isResonance() && event[i2].isFinal())
       || (!event[i1].isFinal() && event[i2].isFinal())) {
       // RF or IF.
       sMax = 2.*p1*p3 + 2.*p1*p2;
     } else if ((event[i1].isFinal() && event[i2].isResonance())
       || (event[i1].isFinal() && !event[i2].isFinal())) {
       // FR or FI.
       sMax = 2.*p2*p3 + 2.*p1*p2;
     } else if (!event[i1].isFinal() || !event[i2].isFinal()) {
       // II.
       sMax = 2.*p1*p2;
     } else {
       loggerPtr->ABORT_MSG("could not determine branching type");
       exit(1);
     }
 
     // Calculate pT2 as in Eq. (5) in arXiv:2008.09468.
     double pT2now = qSq13*qSq23/sMax;
 
     // Sanity check.
     if (pT2now < 0.) {
       loggerPtr->WARNING_MSG("negative pT");
       return -1.;
     }
 
     // Return pT.
     return sqrt(pT2now);
   }
 
   //--------------------------------------------------------------------------
 
   // Compute the POWHEG pT separation between i and j.
   inline double pTpowheg(const Event &e, int i, int j, bool FSR) {
 
     // pT value for FSR and ISR
     double pTnow = 0.;
     if (FSR) {
       // POWHEG d_ij (in CM frame). Note that the incoming beams have not
       // been updated in the parton systems pointer yet (i.e. prior to any
       // potential recoil).
       int iInA = partonSystemsPtr->getInA(0);
       int iInB = partonSystemsPtr->getInB(0);
       double betaZ = - ( e[iInA].pz() + e[iInB].pz() ) /
                        ( e[iInA].e()  + e[iInB].e()  );
       Vec4 iVecBst(e[i].p()), jVecBst(e[j].p());
       iVecBst.bst(0., 0., betaZ);
       jVecBst.bst(0., 0., betaZ);
       pTnow = sqrt( (iVecBst + jVecBst).m2Calc() *
                     iVecBst.e() * jVecBst.e() /
                     pow2(iVecBst.e() + jVecBst.e()) );
 
     } else {
       // POWHEG pT_ISR is just kinematic pT
       pTnow = e[j].pT();
     }
 
     // Check result.
     if (pTnow < 0.) {
       loggerPtr->WARNING_MSG("negative pT");
       return -1.;
     }
 
     return pTnow;
   }
 
   //--------------------------------------------------------------------------
 
   // Calculate pT for a splitting based on pTdefMode.
   // If j is -1, all final-state partons are tried.
   // If i, k, r and xSR are -1, then all incoming and outgoing
   // partons are tried.
   // xSR set to 0 means ISR, while xSR set to 1 means FSR.
   inline double pTcalc(const Event &e, int i, int j, int k, int r, int xSRin) {
 
     // Loop over ISR and FSR if necessary
     double pTemt = -1., pTnow;
     int xSR1 = (xSRin == -1) ? 0 : xSRin;
     int xSR2 = (xSRin == -1) ? 2 : xSRin + 1;
     for (int xSR = xSR1; xSR < xSR2; xSR++) {
       // FSR flag
       bool FSR = (xSR == 0) ? false : true;
 
       // If all necessary arguments have been given, then directly calculate.
       // POWHEG ISR and FSR, need i and j.
       if ((pTdefMode == 0 || pTdefMode == 1) && i > 0 && j > 0) {
         pTemt = pTpowheg(e, i, j, (pTdefMode == 0) ? false : FSR);
 
       // Pythia ISR, need i, j and r.
       } else if (!FSR && pTdefMode == 2 && i > 0 && j > 0 && r > 0) {
         pTemt = pT(e, i, j, r, FSR);
 
       // Pythia FSR, need k, j and r.
       } else if (FSR && pTdefMode == 2 && j > 0 && k > 0 && r > 0) {
         pTemt = pT(e, k, j, r, FSR);
 
       // Otherwise need to try all possible combinations.
       } else {
         // Start by finding incoming legs to the hard system after
         // branching (radiator after branching, i for ISR).
         // Use partonSystemsPtr to find incoming just prior to the
         // branching and track mothers.
         int iInA = partonSystemsPtr->getInA(0);
         int iInB = partonSystemsPtr->getInB(0);
         while (e[iInA].mother1() != 1) { iInA = e[iInA].mother1(); }
         while (e[iInB].mother1() != 2) { iInB = e[iInB].mother1(); }
 
         // If we do not have j, then try all final-state partons.
         int jNow = (j > 0) ? j : 0;
         int jMax = (j > 0) ? j + 1 : e.size();
         for (; jNow < jMax; jNow++) {
 
           // Final-state only.
           if (!e[jNow].isFinal()) continue;
           // Exclude photons (and W/Z!)
           if (QEDvetoMode==0 && e[jNow].colType() == 0) continue;
 
           // POWHEG.
           if (pTdefMode == 0 || pTdefMode == 1) {
 
             // ISR - only done once as just kinematical pT.
             if (!FSR) {
               pTnow = pTpowheg(e, iInA, jNow, (pTdefMode == 0) ? false : FSR);
               if (pTnow > 0.) pTemt = (pTemt < 0) ? pTnow : min(pTemt, pTnow);
 
             // FSR - try all outgoing partons from system before branching
             // as i. Note that for the hard system, there is no
             // "before branching" information.
             } else {
 
               int outSize = partonSystemsPtr->sizeOut(0);
               for (int iMem = 0; iMem < outSize; iMem++) {
                 int iNow = partonSystemsPtr->getOut(0, iMem);
 
                 // i != jNow and no carbon copies
                 if (iNow == jNow ) continue;
                 // Exclude photons (and W/Z!)
                 if (QEDvetoMode==0 && e[iNow].colType() == 0) continue;
                 if (jNow == e[iNow].daughter1()
                   && jNow == e[iNow].daughter2()) continue;
 
                 pTnow = pTpowheg(e, iNow, jNow, (pTdefMode == 0)
                   ? false : FSR);
                 if (pTnow > 0.) pTemt = (pTemt < 0)
                   ? pTnow : min(pTemt, pTnow);
               }
              // for (iMem)
             }
             // if (!FSR)
           // Pythia.
           } else if (pTdefMode == 2) {
 
             // ISR - other incoming as recoiler.
             if (!FSR) {
               pTnow = pT(e, iInA, jNow, iInB, FSR);
               if (pTnow > 0.) pTemt = (pTemt < 0) ? pTnow : min(pTemt, pTnow);
               pTnow = pT(e, iInB, jNow, iInA, FSR);
               if (pTnow > 0.) pTemt = (pTemt < 0) ? pTnow : min(pTemt, pTnow);
 
             // FSR - try all final-state coloured partons as radiator
             //       after emission (k).
             } else {
               for (int kNow = 0; kNow < e.size(); kNow++) {
                 if (kNow == jNow || !e[kNow].isFinal()) continue;
                 if (QEDvetoMode==0 && e[kNow].colType() == 0) continue;
 
                 // For this kNow, need to have a recoiler.
                 // Try two incoming.
                 pTnow = pT(e, kNow, jNow, iInA, FSR);
                 if (pTnow > 0.) pTemt = (pTemt < 0)
                   ? pTnow : min(pTemt, pTnow);
                 pTnow = pT(e, kNow, jNow, iInB, FSR);
                 if (pTnow > 0.) pTemt = (pTemt < 0)
                   ? pTnow : min(pTemt, pTnow);
 
                 // Try all other outgoing.
                 for (int rNow = 0; rNow < e.size(); rNow++) {
                   if (rNow == kNow || rNow == jNow ||
                       !e[rNow].isFinal()) continue;
                   if(QEDvetoMode==0 && e[rNow].colType() == 0) continue;
                   pTnow = pT(e, kNow, jNow, rNow, FSR);
                   if (pTnow > 0.) pTemt = (pTemt < 0)
                     ? pTnow : min(pTemt, pTnow);
                 }
               // for (rNow)
               }
             // for (kNow)
             }
           // if (!FSR)
           }
         // if (pTdefMode)
         }
       // for (j)
       }
     }
     // for (xSR)
 
     return pTemt;
   }
 
   //--------------------------------------------------------------------------
 
   // Extraction of pThard based on the incoming event.
   // Assume that all the final-state particles are in a continuous block
   // at the end of the event and the final entry is the POWHEG emission.
   // If there is no POWHEG emission, then pThard is set to SCALUP.
 
   inline bool canVetoMPIStep()    { return true; }
   inline int  numberVetoMPIStep() { return 1; }
   inline bool doVetoMPIStep(int nMPI, const Event &e) {
     // Extra check on nMPI
     if (nMPI > 1) return false;
     int iEmt = -1;
     double pT1(0.), pTsum(0.);
 
     // When nFinal is set, be strict about comparing the number of final-state
     // particles with expectation from Born and single-real emission states.
     // (Note: the default from 8.309 onwards is nFinal = -1).
     if (nFinal > 0) {
       // Find if there is a POWHEG emission. Go backwards through the
       // event record until there is a non-final particle. Also sum pT and
       // find pT_1 for possible MPI vetoing
       int count = 0;
       for (int i = e.size() - 1; i > 0; i--) {
         if (e[i].isFinal()) {
           count++;
           pT1    = e[i].pT();
           pTsum += e[i].pT();
         } else break;
       }
       // Extra check that we have the correct final state
       if (count != nFinal && count != nFinal + 1) {
         loggerPtr->ABORT_MSG("wrong number of final state particles in event");
         exit(1);
       }
       // Flag if POWHEG radiation present and index
       isEmt = (count == nFinal) ? false : true;
       iEmt  = (isEmt) ? e.size() - 1 : -1;
 
     // If nFinal == -1, then go through the event and extract only the
     // information on the emission and its pT, but do not enforce strict
     // comparisons of final state multiplicity.
     } else {
 
       // Flag whether POWHEG radiation is present, and save index of emission.
       isEmt = false;
       for (int i = e.size() - 1; i > 0; i--) {
         if (e[i].isFinal()) {
           if ( e[i].isParton() && iEmt < 0
             && e[e[i].mother1()].isParton() ) {
             isEmt = true;
             iEmt = i;
           }
           pT1    = e[i].pT();
           pTsum += e[i].pT();
         } else break;
       }
     }
 
     // If there is no radiation or if pThardMode is 0 then set pThard = SCALUP.
     if (!isEmt || pThardMode == 0) {
       pThard = infoPtr->scalup();
 
     // If pThardMode is 1 then the pT of the POWHEG emission is checked against
     // all other incoming and outgoing partons, with the minimal value taken.
     } else if (pThardMode == 1) {
       if (nFinal < 0) {
         loggerPtr->WARNING_MSG(
           "pThard == 1 not available for nFinal == -1, reset pThard = 0.");
         pThardMode = 0;
         pThard = infoPtr->scalup();
       } else {
         pThard = pTcalc(e, -1, iEmt, -1, -1, -1);
       }
 
     // If pThardMode is 2, then the pT of all final-state partons is checked
     // against all other incoming and outgoing partons, with the minimal value
     // taken.
     } else if (pThardMode == 2) {
       if (nFinal < 0) {
         loggerPtr->WARNING_MSG(
           "pThard == 2 not available for nFinal == -1, reset pThard = 0.");
         pThardMode = 0;
         pThard = infoPtr->scalup();
       } else {
         pThard = pTcalc(e, -1, -1, -1, -1, -1);
       }
     }
 
     // Find MPI veto pT if necessary.
     if (MPIvetoMode == 1) {
       pTMPI = (isEmt) ? pTsum / 2. : pT1;
     }
 
     // Initialise other variables.
     accepted   = false;
     nAcceptSeq = nISRveto = nFSRveto = 0;
 
     // Do not veto the event
     return false;
   }
 
   //--------------------------------------------------------------------------
 
   // ISR veto.
 
   inline bool canVetoISREmission() { return (vetoMode == 0) ? false : true; }
   inline bool doVetoISREmission(int, const Event &e, int iSys) {
     // Must be radiation from the hard system
     if (iSys != 0) return false;
 
     // If we already have accepted 'vetoCount' emissions in a row, do nothing
     if (vetoMode == 1 && nAcceptSeq >= vetoCount) return false;
 
     // Pythia radiator after, emitted and recoiler after.
     int iRadAft = -1, iEmt = -1, iRecAft = -1;
     for (int i = e.size() - 1; i > 0; i--) {
       if (showerModel == 1) {
         // Pythia default.
         if      (iRadAft == -1 && e[i].status() == -41) iRadAft = i;
         else if (iEmt    == -1 && e[i].status() ==  43) iEmt    = i;
         else if (iRecAft == -1 && e[i].status() == -42) iRecAft = i;
       } else if (showerModel == 2) {
         // Vincia.
         if      (iRadAft == -1 && e[i].status() == -41) iRadAft = i;
         else if (iEmt    == -1 && e[i].status() ==  43) iEmt    = i;
         else if (iRecAft == -1
           && (e[i].status() == -41 || e[i].status() == 44)) iRecAft = i;
       }
       if (iRadAft != -1 && iEmt != -1 && iRecAft != -1) break;
     }
     if (iRadAft == -1 || iEmt == -1 || iRecAft == -1) {
       loggerPtr->ABORT_MSG("could not find ISR emission");
       exit(1);
     }
 
     // pTemtMode == 0: pT of emitted w.r.t. radiator
     // pTemtMode == 1: min(pT of emitted w.r.t. all incoming/outgoing)
     // pTemtMode == 2: min(pT of all outgoing w.r.t. all incoming/outgoing)
     int xSR      = (pTemtMode == 0) ? 0       : -1;
     int i        = (pTemtMode == 0) ? iRadAft : -1;
     int j        = (pTemtMode != 2) ? iEmt    : -1;
     int k        = -1;
     int r        = (pTemtMode == 0) ? iRecAft : -1;
     double pTemt = pTcalc(e, i, j, k, r, xSR);
 
     // If a Born configuration, and a photon, and QEDvetoMode=2,
     //  then don't veto photons, W, or Z harder than pThard.
     bool vetoParton = (!isEmt && e[iEmt].colType()==0 && QEDvetoMode==2)
       ? false: true;
 
     // Veto if pTemt > pThard.
     if (pTemt > pThard) {
       if(!vetoParton) {
         // Don't veto ANY emissions afterwards.
         nAcceptSeq = vetoCount-1;
       } else {
         nAcceptSeq = 0;
         nISRveto++;
         return true;
       }
     }
 
     // Else mark that an emission has been accepted and continue.
     nAcceptSeq++;
     accepted = true;
     return false;
   }
 
   //--------------------------------------------------------------------------
 
   // FSR veto.
 
   inline bool canVetoFSREmission() { return (vetoMode == 0) ? false : true; }
   inline bool doVetoFSREmission(int, const Event &e, int iSys, bool) {
     // Must be radiation from the hard system.
     if (iSys != 0) return false;
 
     // If we already have accepted 'vetoCount' emissions in a row, do nothing.
     if (vetoMode == 1 && nAcceptSeq >= vetoCount) return false;
 
     // Pythia radiator (before and after), emitted and recoiler (after).
     int iRecAft = e.size() - 1;
     int iEmt    = e.size() - 2;
     int iRadAft = e.size() - 3;
     int iRadBef = e[iEmt].mother1();
     bool stop = false;
     if (showerModel == 2) {
       // Vincia.
       if ( (e[iRecAft].status() != 51 && e[iRecAft].status() != 52) ||
         e[iEmt].status() != 51 || e[iRadAft].status() != 51) stop = true;
     } else {
       // Pythia default.
       if ( (e[iRecAft].status() != 52 && e[iRecAft].status() != -53) ||
         e[iEmt].status() != 51 || e[iRadAft].status() != 51) stop = true;
     }
     if (stop) {
       loggerPtr->ABORT_MSG("could not find FSR emission");
       exit(1);
     }
 
     // Behaviour based on pTemtMode:
     //  0 - pT of emitted w.r.t. radiator before
     //  1 - min(pT of emitted w.r.t. all incoming/outgoing)
     //  2 - min(pT of all outgoing w.r.t. all incoming/outgoing)
     int xSR = (pTemtMode == 0) ? 1       : -1;
     int i   = (pTemtMode == 0) ? iRadBef : -1;
     int k   = (pTemtMode == 0) ? iRadAft : -1;
     int r   = (pTemtMode == 0) ? iRecAft : -1;
 
     // When pTemtMode is 0 or 1, iEmt has been selected.
     double pTemt = 0.;
     if (pTemtMode == 0 || pTemtMode == 1) {
       // Which parton is emitted, based on emittedMode:
       //  0 - Pythia definition of emitted
       //  1 - Pythia definition of radiated after emission
       //  2 - Random selection of emitted or radiated after emission
       //  3 - Try both emitted and radiated after emission
       int j = iRadAft;
       if (emittedMode == 0 || (emittedMode == 2 && rndmPtr->flat() < 0.5)) j++;
 
       for (int jLoop = 0; jLoop < 2; jLoop++) {
         if      (jLoop == 0) pTemt = pTcalc(e, i, j, k, r, xSR);
         else if (jLoop == 1) pTemt = min(pTemt, pTcalc(e, i, j, k, r, xSR));
 
         // For emittedMode == 3, have tried iRadAft, now try iEmt
         if (emittedMode != 3) break;
         if (k != -1) swap(j, k); else j = iEmt;
       }
 
     // If pTemtMode is 2, then try all final-state partons as emitted
     } else if (pTemtMode == 2) {
       pTemt = pTcalc(e, i, -1, k, r, xSR);
 
     }
 
     // If a Born configuration, and a photon, and QEDvetoMode=2,
     //  then don't veto photons, W's or Z's harder than pThard
     bool vetoParton = (!isEmt && e[iEmt].colType()==0 && QEDvetoMode==2)
       ? false: true;
 
     // Veto if pTemt > pThard
     if (pTemt > pThard) {
       if(!vetoParton) {
         // Don't veto ANY emissions afterwards
         nAcceptSeq = vetoCount-1;
       } else {
         nAcceptSeq = 0;
         nFSRveto++;
         return true;
       }
     }
 
     // Else mark that an emission has been accepted and continue
     nAcceptSeq++;
     accepted = true;
     return false;
   }
 
   //--------------------------------------------------------------------------
 
   // MPI veto.
 
   inline bool canVetoMPIEmission() {return (MPIvetoMode == 0) ? false : true;}
   inline bool doVetoMPIEmission(int, const Event &e) {
     if (MPIvetoMode == 1) {
       if (e[e.size() - 1].pT() > pTMPI) return true;
     }
     return false;
   }
 
   //--------------------------------------------------------------------------
 
   // Functions to return information.
 
   inline int getNISRveto() { return nISRveto; }
   inline int getNFSRveto() { return nFSRveto; }
 
   //--------------------------------------------------------------------------
 
  protected:
   double pThard, pTMPI;
 
  private:
   int    showerModel, nFinal, vetoMode, MPIvetoMode, QEDvetoMode, vetoCount;
   int    pThardMode, pTemtMode, emittedMode, pTdefMode;
   bool   accepted, isEmt;
   // The number of accepted emissions (in a row)
   // Flag for PowHeg Born or Radiation
   int nAcceptSeq;
   // Statistics on vetos
   unsigned long int nISRveto, nFSRveto;
 
 };
 
 //--------------------------------------------------------------------------
 
 // Declare the plugin.
 
 PYTHIA8_PLUGIN_CLASS(UserHooks, PowhegHooks, false, false, false)
 PYTHIA8_PLUGIN_VERSIONS(PYTHIA_VERSION_INTEGER)
 
 //==========================================================================
 
 } // end namespace Pythia8
 
 #endif // end Pythia8_PowhegHooks_H

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