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Rivet analyses reference

BABAR_2009_I819092

Mass distributions and ˉΛ0 polarization in B0ˉΛ0pπ
Experiment: BABAR (PEP-II)
Inspire ID: 819092
Status: VALIDATED NOHEPDATA
Authors:
  • Peter Richardson
References:
  • Phys.Rev.D 79 (2009) 112009
Beams: * *
Beam energies: ANY
Run details:
  • Any process producing B0 mesons, originally Upsilon(4S) decays

Measurement of the ˉΛ0p mass spectrum and ˉΛ0 energy in the decay B0ˉΛ0pπ. The polarization of the ˉΛ0 is also measured. The data were read from the plots/tables in the paper but are efficiency corrected and background subtracted. In additon the values of the polarization were adjusted to use the PDG 2022 value of αΛ as there has been a significant change due to due measuremnts.

Source code: BABAR_2009_I819092.cc
  1// -*- C++ -*-
  2#include "Rivet/Analysis.hh"
  3#include "Rivet/Projections/UnstableParticles.hh"
  4#include "Rivet/Projections/DecayedParticles.hh"
  5
  6namespace Rivet {
  7
  8
  9  /// @brief B0 -> lambdabar p pi-
 10  class BABAR_2009_I819092 : public Analysis {
 11  public:
 12
 13    /// Constructor
 14    RIVET_DEFAULT_ANALYSIS_CTOR(BABAR_2009_I819092);
 15
 16
 17    /// @name Analysis methods
 18    /// @{
 19
 20    /// Book histograms and initialise projections before the run
 21    void init() {
 22      // Initialise and register projections
 23      UnstableParticles ufs = UnstableParticles(Cuts::pid==511);
 24      declare(ufs, "UFS");
 25      DecayedParticles B0(ufs);
 26      B0.addStable( 3122);
 27      B0.addStable(-3122);
 28      declare(B0, "B0");
 29      book(_h_pol1,2,1,1);
 30      for(unsigned int ix=0;ix<3;++ix) {
 31	if(ix<2) book(_h_mass[ix],1,1,1+ix);
 32	book(_h_pol2[ix],3,1,1+ix);
 33      }
 34    }
 35
 36
 37    /// Perform the per-event analysis
 38    void analyze(const Event& event) {
 39      double alpha = -0.732;
 40      static const map<PdgId,unsigned int> & mode   = { { 2212,1},{-3122,1}, {-211,1}};
 41      DecayedParticles B0 = apply<DecayedParticles>(event, "B0");
 42      // loop over particles
 43      for(unsigned int ix=0;ix<B0.decaying().size();++ix) {
 44	if (!B0.modeMatches(ix,3,mode)) continue;
 45       	const Particle & pp     = B0.decayProducts()[ix].at( 2212)[0];
 46       	const Particle & LamBar = B0.decayProducts()[ix].at(-3122)[0];
 47	_h_mass[0]->fill( (pp.momentum()+LamBar.momentum()).mass());
 48	// boost to B rest frame
 49	LorentzTransform boost =
 50	  LorentzTransform::mkFrameTransformFromBeta(B0.decaying()[ix]. momentum().betaVec());
 51	FourMomentum pLam    = boost.transform(LamBar.momentum());
 52	FourMomentum pProton = boost.transform(pp    .momentum());
 53	_h_mass[1]->fill(pLam.E());
 54	// Lambda decay products
 55	if(LamBar.children().size()!=2) continue;
 56	Particle pbar;
 57	if(LamBar.children()[0].pid()==-2212 &&
 58	   LamBar.children()[1].pid()== 211) {
 59	  pbar = LamBar.children()[0];
 60	}
 61	else if(LamBar.children()[1].pid()==-2212 &&
 62		LamBar.children()[0].pid()== 211) {
 63	  pbar = LamBar.children()[1];
 64	}
 65	else
 66	  continue;
 67	LorentzTransform boost2 = LorentzTransform::mkFrameTransformFromBeta(pLam.betaVec());
 68	Vector3 axisP = boost2.transform(boost.transform(pbar.momentum())).p3().unit();
 69	Vector3 axis1 = pLam.p3().unit();
 70	double cTheta = axisP.dot(axis1);
 71	_h_pol1   ->fill(pLam.E(),3.*cTheta);
 72	_h_pol2[0]->fill(pLam.E(),3.*cTheta/alpha);
 73	Vector3 axis2 = pLam.p3().cross(pProton.p3()).unit();
 74	cTheta = axisP.dot(axis2);
 75	_h_pol2[1]->fill(pLam.E(),3.*cTheta/alpha);
 76	Vector3 axis3 = axis1.cross(axis2);
 77	cTheta = axisP.dot(axis3);
 78	_h_pol2[2]->fill(pLam.E(),3.*cTheta/alpha);
 79      }
 80    }
 81
 82
 83    /// Normalise histograms etc., after the run
 84    void finalize() {
 85      for(unsigned int ix=0;ix<2;++ix)
 86	normalize(_h_mass[ix],1.,false);
 87    }
 88
 89    /// @}
 90
 91
 92    /// @name Histograms
 93    /// @{
 94    Histo1DPtr _h_mass[2];
 95    Profile1DPtr _h_pol1,_h_pol2[3];
 96    /// @}
 97
 98
 99  };
100
101
102  RIVET_DECLARE_PLUGIN(BABAR_2009_I819092);
103
104}