Rivet analyses

Kinematic distributions in D⁰ → π⁻π⁰e⁺ν_e and D⁺ → π⁺π⁻e⁺ν_e

Experiment: CLEO (CESR)

Inspire ID: 1081165

Status: VALIDATED NOHEPDATA

Authors: - Peter Richardson

References: - Phys.Rev.Lett. 110 (2013) 13, 131802

Beams: * *

Beam energies: ANY

Run details: - Any process producing D0 or D+

Measurement of the kinematic distributions in D⁰ → π⁻π⁰e⁺ν_e and D⁺ → π⁺π⁻e⁺ν_e by CLEO. N.B. the plots where read from the paper and may not have been corrected for acceptance.

Source code:`CLEO_2013_I1081165.cc`

// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/DecayedParticles.hh"
#include "Rivet/Projections/UnstableParticles.hh"

namespace Rivet {


  /// @brief D -> rho e nu
  class CLEO_2013_I1081165 : public Analysis {
  public:

    /// Constructor
    RIVET_DEFAULT_ANALYSIS_CTOR(CLEO_2013_I1081165);


    /// @name Analysis methods
    /// @{

    /// Book histograms and initialise projections before the run
    void init() {
      // Initialise and register projections
      UnstableParticles ufs = UnstableParticles(Cuts::pid == 411 || Cuts::pid == 421);
      declare(ufs, "UFS");
      DecayedParticles DD(ufs);
      DD.addStable(PID::PI0);
      DD.addStable(PID::K0S);
      DD.addStable(PID::ETA);
      DD.addStable(PID::ETAPRIME);
      declare(DD, "DD");

      // Book histograms
      for (unsigned int ix = 0; ix < 4; ++ix) book(_h[ix], 1, 1, 1 + ix);
    }


    /// Perform the per-event analysis
    void analyze(const Event& event) {
      static const map<PdgId, unsigned int>& mode1 = {{111, 1}, {-211, 1}, {-11, 1}, {12, 1}};
      static const map<PdgId, unsigned int>& mode2 = {{211, 1}, {-211, 1}, {-11, 1}, {12, 1}};
      DecayedParticles DD = apply<DecayedParticles>(event, "DD");
      // loop over particles
      for (unsigned int ix = 0; ix < DD.decaying().size(); ++ix) {
        Particle pi2;
        if (DD.decaying()[ix].pid() == 421 && DD.modeMatches(ix, 4, mode1)) {
          pi2 = DD.decayProducts()[ix].at(111)[0];
        }
        else if (DD.decaying()[ix].pid() == 411 && DD.modeMatches(ix, 4, mode2)) {
          pi2 = DD.decayProducts()[ix].at(211)[0];
        }
        else
          continue;
        const Particle& pim = DD.decayProducts()[ix].at(-211)[0];
        const Particle& ep = DD.decayProducts()[ix].at(-11)[0];
        const Particle& nue = DD.decayProducts()[ix].at(12)[0];
        FourMomentum pRho = pi2.momentum() + pim.momentum();
        if (abs(pRho.mass() - 0.7753) > 0.15) continue;
        FourMomentum qq = DD.decaying()[ix].momentum() - pRho;
        _h[0]->fill(qq.mass2());
        // boost momenta to D rest frame
        LorentzTransform boost = LorentzTransform::mkFrameTransformFromBeta(
            DD.decaying()[ix].momentum().betaVec());
        FourMomentum pPP = boost.transform(pRho);
        Matrix3 ptoz(-pPP.p3().unit(), Vector3(0, 0, 1));
        boost.preMult(ptoz);
        // the momenta in frane to W along z
        FourMomentum pD = boost.transform(DD.decaying()[ix].momentum());
        FourMomentum ppi2 = boost.transform(pi2.momentum());
        FourMomentum ppim = boost.transform(pim.momentum());
        FourMomentum pe = boost.transform(ep.momentum());
        FourMomentum pnu = boost.transform(nue.momentum());
        pRho = ppi2 + ppim;
        qq = pD - pRho;
        LorentzTransform boostRho = LorentzTransform::mkFrameTransformFromBeta(pRho.betaVec());
        Vector3 axisRho = boostRho.transform(ppim).p3().unit();
        _h[1]->fill(axisRho.dot(pRho.p3().unit()));
        LorentzTransform boostW = LorentzTransform::mkFrameTransformFromBeta(qq.betaVec());
        Vector3 axisE = boostW.transform(pe).p3().unit();
        _h[2]->fill(axisE.dot(qq.p3().unit()));
        axisRho.setZ(0.);
        axisE.setZ(0.);
        double chi = atan2(axisE.cross(axisRho).dot(qq.p3().unit()), axisE.dot(axisRho));
        _h[3]->fill(chi);
      }
    }


    /// Normalise histograms etc., after the run
    void finalize() {
      for (unsigned int ix = 0; ix < 4; ++ix) normalize(_h[ix]);
    }

    /// @}


    /// @name Histograms
    /// @{
    Histo1DPtr _h[4];
    /// @}
  };


  RIVET_DECLARE_PLUGIN(CLEO_2013_I1081165);

}

Rivet analyses

Kinematic distributions in D0 → π−π0e+νe and D+ → π+π−e+νe

Source code:CLEO_2013_I1081165.cc

Kinematic distributions in D⁰ → π⁻π⁰e⁺ν_e and D⁺ → π⁺π⁻e⁺ν_e

Source code:`CLEO_2013_I1081165.cc`