## main468

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    // main468.cc is a part of the PYTHIA event generator.
    // Copyright (C) 2025 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.

    // Authors:
    //            Marius Utheim
    //            Philip Ilten

    // Keywords:
    //            Low energy
    //            Resonances

    // Illustration of how to create new resonance particles that can form
    // during rescattering. The resonances are exotic hadrons defined in
    // main468.cmnd. The resulting invariant mass spectra are plotted, but the
    // exotic hadrons are rare and statistics are low, even with 100k events.

    #include "Pythia8/Pythia.h"

    using namespace Pythia8;

    //==========================================================================

    int main() {

      // Number of events. In 100k events, we expect a handful of T(2900)
      // tetraquarks, a few chi_1c(3872) tetraquarks, and possibly a few
      // P_c^+ pentaquarks.
      int nEvent = 100000;

      // Initialize Pythia.
      Pythia pythia;
      Event& event = pythia.event;

      // Read file for exotic hadron definitions.
      pythia.readFile("main468.cmnd");

      // Run configuration. Charmonium processes favour production of the
      // relevant exotic hadrons.
      pythia.readString("Charmonium:all = on");
      pythia.readString("Beams:eCM = 13000");

      // Enable rescattering. Retune pT0Ref to get correct charged multiplicity.
      pythia.readString("HadronLevel:rescatter = on");
      pythia.readString("MultipartonInteractions:pT0Ref = 2.345");

      // Initialize.
      if (!pythia.init()) {
        cout << " Pythia failed to initialize." << endl;
        return 1;
      }

      // Exotic hadron mass spectra.
      Hist mX3872("chi_1c(3872)",  30, 3.82, 3.92);

      Hist mTcs0("T_0cs(2900)0",        30, 2.2, 3.6);
      Hist mTcs1("T_1cs(2900)0",        30, 2.2, 3.6);
      Hist mTcsbar0("T_csbar(2900)0",   30, 2.2, 3.6);
      Hist mTcsbarPP("T_csbar(2900)++", 30, 2.2, 3.6);

      Hist mPc4312("P_c(4312)+", 30, 4.2, 4.6);
      Hist mPc4440("P_c(4440)+", 30, 4.2, 4.6);
      Hist mPc4457("P_c(4457)+", 30, 4.2, 4.6);

      // Generate events.
      int nSuccess = 0;
      for (int iEvent = 0; iEvent < nEvent; ++iEvent) {
        if (!pythia.next())
          continue;
        nSuccess += 1;

        // Loop over event record and find tetraquarks.
        for (Particle& h : event) {
          if      (h.idAbs() == 9044111) mX3872.fill(h.m());
          else if (h.idAbs() == 9043211) mTcs0.fill(h.m());
          else if (h.idAbs() == 9043212) mTcs1.fill(h.m());
          else if (h.idAbs() == 9043213) mTcsbar0.fill(h.m());
          else if (h.idAbs() == 9043214) mTcsbarPP.fill(h.m());
          else if (h.idAbs() == 9422141) mPc4312.fill(h.m());
          else if (h.idAbs() == 9422142) mPc4440.fill(h.m());
          else if (h.idAbs() == 9422143) mPc4457.fill(h.m());
        }

      }

      // Normalize and calculate production cross sections.
      double sigGen = pythia.info.sigmaGen();
      mX3872.normalizeSpectrum(nSuccess); mX3872 *= sigGen;
      mTcs0.normalizeSpectrum(nSuccess); mTcs0 *= sigGen;
      mTcs1.normalizeSpectrum(nSuccess); mTcs1 *= sigGen;
      mTcsbar0.normalizeSpectrum(nSuccess); mTcsbar0 *= sigGen;
      mTcsbarPP.normalizeSpectrum(nSuccess); mTcsbarPP *= sigGen;
      mPc4312.normalizeSpectrum(nSuccess); mPc4312 *= sigGen;
      mPc4440.normalizeSpectrum(nSuccess); mPc4440 *= sigGen;
      mPc4457.normalizeSpectrum(nSuccess); mPc4457 *= sigGen;

      // Plot.
      string plotName = "fig468";
      HistPlot plt("plot468");

      // Plot production cross sections for T(2900) tetraquarks.
      plt.frame(plotName, "$T(2900)$ tetraquark production cross sections",
        "$E_{CM}$ [GeV]", "$\\sigma$ [mb]");
      plt.add(Hist::plotFunc([&](double eCM) {
        return pythia.getSigmaPartial(-411, 321, eCM, 9043211);
      }, "", 200, 2.2, 3.6), "-", "$\\bar{D}^- K^+ \\to T_{cs0}(2900)^0$");
      plt.add(Hist::plotFunc([&](double eCM) {
        return pythia.getSigmaPartial(-411, 321, eCM, 9043212);
      }, "", 200, 2.2, 3.6), "-", "$\\bar{D}^- K^+ \\to T_{cs1}(2900)^0$");
      plt.add(Hist::plotFunc([&](double eCM) {
        return pythia.getSigmaPartial(431, -211, eCM, 9043213);
      }, "", 200, 2.2, 3.6), "-", "$D_s^+ \\pi^- \\to T_{c\\bar{s}}^a(2900)^0$");
      plt.add(Hist::plotFunc([&](double eCM) {
        return pythia.getSigmaPartial(431,  211, eCM, 9043214);
      }, "", 200, 2.2, 3.6), "-",
        "$D_s^+ \\pi^+ \\to T_{c\\bar{s}}^a(2900)^{++}$");
      plt.plot();

      // Plot invariant mass spectra.
      plt.frame(plotName, "$T(2900)$ tetraquark invariant mass spectra",
        "$m$ [GeV]", "$d\\sigma/dm$");
      plt.add(mTcs0, "h", "$T_{cs0}(2900)^0$");
      plt.add(mTcs1,  "h", "$T_{cs1}(2900)^0$");
      plt.add(mTcsbar0, "h", "$T_{c\\bar{s}}^a(2900)^0$");
      plt.add(mTcsbarPP, "h", "$T_{c\\bar{s}}^a(2900)^{++}$");
      plt.plot();

      plt.frame(plotName, "$\\chi_{c1}(3872)$ invariant mass spectra",
        "$m$ [GeV]", "$d\\sigma/dm$");
      plt.add(mX3872, "h", "$X(3872)$");
      plt.plot();

      plt.frame(plotName, "$P_c$ invariant mass spectra",
        "$m$ [GeV]", "$d\\sigma/dm$");
      plt.add(mPc4312, "h", "$P_c^+(4312)$");
      plt.add(mPc4440, "h", "$P_c^+(4440)$");
      plt.add(mPc4457, "h", "$P_c^+(4457)$");
      plt.plot();

      // Print statistics and done.
      pythia.stat();
      return 0;
    }