Computes neutrino-nucleon(nucleus) QELCC differential cross section Is a concrete implementation of the XSecAlgorithmI interface.
. More...

#include <LwlynSmithQELCCPXSec.h>

Inheritance diagram for genie::LwlynSmithQELCCPXSec:

Public Member Functions
	LwlynSmithQELCCPXSec ()

	LwlynSmithQELCCPXSec (string config)

virtual	~LwlynSmithQELCCPXSec ()

double	XSec (const Interaction *i, KinePhaseSpace_t k) const
	Compute the cross section for the input interaction. More...

double	Integral (const Interaction *i) const

bool	ValidProcess (const Interaction *i) const
	Can this cross section algorithm handle the input process? More...

void	Configure (const Registry &config)

void	Configure (string param_set)

Public Member Functions inherited from genie::XSecAlgorithmI
virtual	~XSecAlgorithmI ()

virtual bool	ValidKinematics (const Interaction *i) const
	Is the input kinematical point a physically allowed one? More...

Public Member Functions inherited from genie::Algorithm
virtual	~Algorithm ()

virtual void	FindConfig (void)

virtual const Registry &	GetConfig (void) const

Registry *	GetOwnedConfig (void)

virtual const AlgId &	Id (void) const
	Get algorithm ID. More...

virtual AlgStatus_t	GetStatus (void) const
	Get algorithm status. More...

virtual bool	AllowReconfig (void) const

virtual AlgCmp_t	Compare (const Algorithm *alg) const
	Compare with input algorithm. More...

virtual void	SetId (const AlgId &id)
	Set algorithm ID. More...

virtual void	SetId (string name, string config)

const Algorithm *	SubAlg (const RgKey &registry_key) const

void	AdoptConfig (void)

void	AdoptSubstructure (void)

virtual void	Print (ostream &stream) const
	Print algorithm info. More...

Private Member Functions
double	FullDifferentialXSec (const Interaction *i) const

void	LoadConfig (void)

Private Attributes
QELFormFactors	fFormFactors

const QELFormFactorsModelI *	fFormFactorsModel

const XSecIntegratorI *	fXSecIntegrator

double	fCos8c2
	cos^2(cabibbo angle) More...

double	fXSecScale
	external xsec scaling factor More...

const NuclearModelI *	fNuclModel

bool	fLFG
	If the nuclear model is lfg alway average over nucleons. More...

bool	fDoAvgOverNucleonMomentum
	Average cross section over hit nucleon monentum? More...

double	fEnergyCutOff

QELEvGen_BindingMode_t	fIntegralNucleonBindingMode

bool	fDoPauliBlocking
	Whether to apply Pauli blocking in FullDifferentialXSec. More...

const genie::PauliBlocker *	fPauliBlocker
	The PauliBlocker instance to use to apply that correction. More...

Additional Inherited Members
Static Public Member Functions inherited from genie::Algorithm
static string	BuildParamVectKey (const std::string &comm_name, unsigned int i)

static string	BuildParamVectSizeKey (const std::string &comm_name)

Protected Member Functions inherited from genie::XSecAlgorithmI
	XSecAlgorithmI ()

	XSecAlgorithmI (string name)

	XSecAlgorithmI (string name, string config)

Protected Member Functions inherited from genie::Algorithm
	Algorithm ()

	Algorithm (string name)

	Algorithm (string name, string config)

void	Initialize (void)

void	DeleteConfig (void)

void	DeleteSubstructure (void)

Registry *	ExtractLocalConfig (const Registry &in) const

Registry *	ExtractLowerConfig (const Registry &in, const string &alg_key) const
	Split an incoming configuration Registry into a block valid for the sub-algo identified by alg_key. More...

template<class T >
bool	GetParam (const RgKey &name, T &p, bool is_top_call=true) const

template<class T >
bool	GetParamDef (const RgKey &name, T &p, const T &def) const

template<class T >
int	GetParamVect (const std::string &comm_name, std::vector< T > &v, bool is_top_call=true) const
	Handle to load vectors of parameters. More...

int	GetParamVectKeys (const std::string &comm_name, std::vector< RgKey > &k, bool is_top_call=true) const

int	AddTopRegistry (Registry *rp, bool owns=true)
	add registry with top priority, also update ownership More...

int	AddLowRegistry (Registry *rp, bool owns=true)
	add registry with lowest priority, also update ownership More...

int	MergeTopRegistry (const Registry &r)

int	AddTopRegisties (const vector< Registry * > &rs, bool owns=false)
	Add registries with top priority, also udated Ownerships. More...

Protected Attributes inherited from genie::Algorithm
bool	fAllowReconfig

bool	fOwnsSubstruc
	true if it owns its substructure (sub-algs,...) More...

AlgId	fID
	algorithm name and configuration set More...

vector< Registry * >	fConfVect

vector< bool >	fOwnerships
	ownership for every registry in fConfVect More...

AlgStatus_t	fStatus
	algorithm execution status More...

AlgMap *	fOwnedSubAlgMp
	local pool for owned sub-algs (taken out of the factory pool) More...

Detailed Description

Computes neutrino-nucleon(nucleus) QELCC differential cross section Is a concrete implementation of the XSecAlgorithmI interface.
.

C.H.Llewellyn Smith, Physics Reports (Sect. C of Physics Letters) 3, No. 5 (1972) 261-379

Author: Costas Andreopoulos <constantinos.andreopoulos cern.ch> University of Liverpool & STFC Rutherford Appleton Laboratory

May 05, 2004

Definition at line 37 of file LwlynSmithQELCCPXSec.h.

Constructor & Destructor Documentation

LwlynSmithQELCCPXSec::LwlynSmithQELCCPXSec ( )

Definition at line 41 of file LwlynSmithQELCCPXSec.cxx.

                                            :
 XSecAlgorithmI("genie::LwlynSmithQELCCPXSec")
 {
 
 }

LwlynSmithQELCCPXSec::LwlynSmithQELCCPXSec ( string config )

Definition at line 47 of file LwlynSmithQELCCPXSec.cxx.

                                                         :
 XSecAlgorithmI("genie::LwlynSmithQELCCPXSec", config)
 {
 
 }

LwlynSmithQELCCPXSec::~LwlynSmithQELCCPXSec ( )

virtual

Definition at line 53 of file LwlynSmithQELCCPXSec.cxx.

 {
 
 }

Member Function Documentation

void LwlynSmithQELCCPXSec::Configure ( const Registry & config )

virtual

Configure the algorithm with an external registry The registry is merged with the top level registry if it is owned, Otherwise a copy of it is added with the highest priority

Reimplemented from genie::Algorithm.

Definition at line 402 of file LwlynSmithQELCCPXSec.cxx.

 {
   Algorithm::Configure(config);
   this->LoadConfig();
 }

void LwlynSmithQELCCPXSec::Configure ( string config )

virtual

Configure the algorithm from the AlgoConfigPool based on param_set string given in input An algorithm contains a vector of registries coming from different xml configuration files, which are loaded according a very precise prioriy This methods will load a number registries in order of priority: 1) "Tunable" parameter set from CommonParametes. This is loaded with the highest prioriry and it is designed to be used for tuning procedure Usage not expected from the user. 2) For every string defined in "CommonParame" the corresponding parameter set will be loaded from CommonParameter.xml 3) parameter set specified by the config string and defined in the xml file of the algorithm 4) if config is not "Default" also the Default parameter set from the same xml file will be loaded Effectively this avoids the repetion of a parameter when it is not changed in the requested configuration

Reimplemented from genie::Algorithm.

Definition at line 408 of file LwlynSmithQELCCPXSec.cxx.

 {
   Algorithm::Configure(config);
   this->LoadConfig();
 }

double LwlynSmithQELCCPXSec::FullDifferentialXSec ( const Interaction * i ) const

private

Definition at line 164 of file LwlynSmithQELCCPXSec.cxx.

 {
   // First we need access to all of the particles in the interaction
   // The particles were stored in the lab frame
   const Kinematics&   kinematics = interaction -> Kine();
   const InitialState& init_state = interaction -> InitState();
 
   const Target& tgt = init_state.Tgt();
 
   const TLorentzVector leptonMom = kinematics.FSLeptonP4();
   const TLorentzVector outNucleonMom = kinematics.HadSystP4();
 
   // Apply Pauli blocking if enabled
   if ( fDoPauliBlocking && tgt.IsNucleus() && !interaction->TestBit(kIAssumeFreeNucleon) ) {
     int final_nucleon_pdg = interaction->RecoilNucleonPdg();
     double kF = fPauliBlocker->GetFermiMomentum(tgt, final_nucleon_pdg,
       tgt.HitNucPosition());
     double pNf = outNucleonMom.P();
     if ( pNf < kF ) return 0.;
   }
 
   // Note that GetProbeP4 defaults to returning the probe 4-momentum in the
   // struck nucleon rest frame, so we have to explicitly ask for the lab frame
   // here
   TLorentzVector * tempNeutrino = init_state.GetProbeP4(kRfLab);
   TLorentzVector neutrinoMom = *tempNeutrino;
   delete tempNeutrino;
   TLorentzVector * inNucleonMom = init_state.TgtPtr()->HitNucP4Ptr();
 
   // *** CALCULATION OF "q" and "qTilde" ***
   // According to the de Forest prescription for handling the off-shell
   // initial struck nucleon, the cross section calculation should proceed
   // as if for a free nucleon, except that an effective value of the 4-momentum
   // transfer qTilde should be used in which the difference between the on-
   // and off-shell energies of the hit nucleon has been subtracted from the
   // energy transfer q0.
 
   // HitNucMass() looks up the PDGLibrary (on-shell) value for the initial
   // struck nucleon
   double mNi = init_state.Tgt().HitNucMass();
 
   // Hadronic matrix element for CC neutrino interactions should really use
   // the "nucleon mass," i.e., the mean of the proton and neutrino masses.
   // This expression would also work for NC and EM scattering (since the
   // initial and final on-shell nucleon masses would be the same)
   double mNucleon = ( mNi + interaction->RecoilNucleon()->Mass() ) / 2.;
 
   // Ordinary 4-momentum transfer
   TLorentzVector qP4 = neutrinoMom - leptonMom;
 
   // Initial struck nucleon 4-momentum in which it is forced to be on-shell
   double inNucleonOnShellEnergy = std::sqrt( std::pow(mNi, 2)
     + std::pow(inNucleonMom->P(), 2) );
   TLorentzVector inNucleonMomOnShell( inNucleonMom->Vect(), inNucleonOnShellEnergy );
 
   // Effective 4-momentum transfer (according to the deForest prescription) for
   // use in computing the hadronic tensor
   TLorentzVector qTildeP4 = outNucleonMom - inNucleonMomOnShell;
 
   double Q2 = -1. * qP4.Mag2();
   double Q2tilde = -1. * qTildeP4.Mag2();
 
   // If the binding energy correction causes an unphysical value
   // of q0Tilde or Q2tilde, just return 0.
   if ( qTildeP4.E() <= 0. && init_state.Tgt().IsNucleus() &&
     !interaction->TestBit(kIAssumeFreeNucleon) ) return 0.;
   if ( Q2tilde <= 0. ) return 0.;
 
   // Store Q2tilde in the kinematic variable representing Q2.
   // This will ensure that the form factors are calculated correctly
   // using the de Forest prescription (Q2tilde instead of Q2).
   interaction->KinePtr()->SetQ2(Q2tilde);
 
   // Calculate the QEL form factors
   fFormFactors.Calculate(interaction);
 
   double F1V   = fFormFactors.F1V();
   double xiF2V = fFormFactors.xiF2V();
   double FA    = fFormFactors.FA();
   double Fp    = fFormFactors.Fp();
 
   // Restore Q2 in the interaction's kinematic variables
   // now that the form factors have been computed
   interaction->KinePtr()->SetQ2( Q2 );
 
   // Overall factor in the differential cross section
   double Gfactor = kGF2*fCos8c2 / ( 8. * kPi * kPi * inNucleonOnShellEnergy
     * neutrinoMom.E() * outNucleonMom.E() * leptonMom.E() );
 
   // Now, we can calculate the cross section
   double tau = Q2tilde / (4 * std::pow(mNucleon, 2));
   double h1 = FA*FA*(1 + tau) + tau*(F1V + xiF2V)*(F1V + xiF2V);
   double h2 = FA*FA + F1V*F1V + tau*xiF2V*xiF2V;
   double h3 = 2.0 * FA * (F1V + xiF2V);
   double h4 = 0.25 * xiF2V*xiF2V *(1-tau) + 0.5*F1V*xiF2V + FA*Fp - tau*Fp*Fp;
 
   bool is_neutrino = pdg::IsNeutrino(init_state.ProbePdg());
   int sign = (is_neutrino) ? -1 : 1;
   double l1 = 2*neutrinoMom.Dot(leptonMom)*std::pow(mNucleon, 2);
   double l2 = 2*(neutrinoMom.Dot(inNucleonMomOnShell)) * (inNucleonMomOnShell.Dot(leptonMom)) - neutrinoMom.Dot(leptonMom)*std::pow(mNucleon, 2);
   double l3 = (neutrinoMom.Dot(inNucleonMomOnShell) * qTildeP4.Dot(leptonMom)) - (neutrinoMom.Dot(qTildeP4) * leptonMom.Dot(inNucleonMomOnShell));
   l3 *= sign;
   double l4 = neutrinoMom.Dot(leptonMom) * qTildeP4.Dot(qTildeP4) - 2*neutrinoMom.Dot(qTildeP4)*leptonMom.Dot(qTildeP4);
   double l5 = neutrinoMom.Dot(inNucleonMomOnShell) * leptonMom.Dot(qTildeP4) + leptonMom.Dot(inNucleonMomOnShell)*neutrinoMom.Dot(qTildeP4) - neutrinoMom.Dot(leptonMom)*inNucleonMomOnShell.Dot(qTildeP4);
 
   double LH = 2 *(l1*h1 + l2*h2 + l3*h3 + l4*h4 + l5*h2);
 
   double xsec = Gfactor * LH;
 
   // Apply the factor that arises from elimination of the energy-conserving
   // delta function
   xsec *= genie::utils::EnergyDeltaFunctionSolutionQEL( *interaction );
 
   // Apply given scaling factor
   xsec *= fXSecScale;
 
   // Number of scattering centers in the target
   const Target & target = init_state.Tgt();
   int nucpdgc = target.HitNucPdg();
   int NNucl = (pdg::IsProton(nucpdgc)) ? target.Z() : target.N();
 
 #ifdef __GENIE_LOW_LEVEL_MESG_ENABLED__
   LOG("LwlynSmith", pDEBUG)
     << "Nuclear suppression factor R(Q2) = " << R << ", NNucl = " << NNucl;
 #endif
 
   xsec *= NNucl; // nuclear xsec
 
   return xsec;
 
 }

double LwlynSmithQELCCPXSec::Integral ( const Interaction * i ) const

virtual

Integrate the model over the kinematic phase space available to the input interaction (kinematical cuts can be included)

Implements genie::XSecAlgorithmI.

Definition at line 297 of file LwlynSmithQELCCPXSec.cxx.

 {
   // If we're using the new spline generation method (which integrates
   // over the kPSQELEvGen phase space used by QELEventGenerator) then
   // let the cross section integrator do all of the work. It's smart
   // enough to handle free nucleon vs. nuclear targets, different
   // nuclear models (including the local Fermi gas model), etc.
   // TODO: think about doing this in a better way
   if ( fXSecIntegrator->Id().Name() == "genie::NewQELXSec" ) {
     return fXSecIntegrator->Integrate(this, in);
   }
 
   // Otherwise, use the old integration method (kept for use with
   // the historical default G18_00x series of tunes)
   bool nuclear_target = in->InitState().Tgt().IsNucleus();
   if(!nuclear_target || !fDoAvgOverNucleonMomentum) {
     return fXSecIntegrator->Integrate(this,in);
   }
 
   double E = in->InitState().ProbeE(kRfHitNucRest);
   if(fLFG || E < fEnergyCutOff) {
     // clone the input interaction so as to tweak the
     // hit nucleon 4-momentum in the averaging loop
     Interaction in_curr(*in);
 
     // hit target
     Target * tgt = in_curr.InitState().TgtPtr();
 
     // get nuclear masses (init & final state nucleus)
     int nucleon_pdgc = tgt->HitNucPdg();
     bool is_p = pdg::IsProton(nucleon_pdgc);
     int Zi = tgt->Z();
     int Ai = tgt->A();
     int Zf = (is_p) ? Zi-1 : Zi;
     int Af = Ai-1;
     PDGLibrary * pdglib = PDGLibrary::Instance();
     TParticlePDG * nucl_i = pdglib->Find( pdg::IonPdgCode(Ai, Zi) );
     TParticlePDG * nucl_f = pdglib->Find( pdg::IonPdgCode(Af, Zf) );
     if(!nucl_f) {
       LOG("LwlynSmith", pFATAL)
         << "Unknwown nuclear target! No target with code: "
         << pdg::IonPdgCode(Af, Zf) << " in PDGLibrary!";
       exit(1);
     }
     double Mi  = nucl_i -> Mass(); // initial nucleus mass
     double Mf  = nucl_f -> Mass(); // remnant nucleus mass
 
     // throw nucleons with fermi momenta and binding energies
     // generated according to the current nuclear model for the
     // input target and average the cross section
     double xsec_sum = 0.;
     const int nnuc = 2000;
     // VertexGenerator for generating a position before generating
     // each nucleon
     VertexGenerator * vg = new VertexGenerator();
     vg->Configure("Default");
     for(int inuc=0;inuc<nnuc;inuc++){
       // Generate a position in the nucleus
       TVector3 nucpos = vg->GenerateVertex(&in_curr,tgt->A());
       tgt->SetHitNucPosition(nucpos.Mag());
 
       // Generate a nucleon
       fNuclModel->GenerateNucleon(*tgt, nucpos.Mag());
       TVector3 p3N = fNuclModel->Momentum3();
       double   EN  = Mi - TMath::Sqrt(p3N.Mag2() + Mf*Mf);
       TLorentzVector* p4N = tgt->HitNucP4Ptr();
       p4N->SetPx (p3N.Px());
       p4N->SetPy (p3N.Py());
       p4N->SetPz (p3N.Pz());
       p4N->SetE  (EN);
 
       double xsec = fXSecIntegrator->Integrate(this,&in_curr);
       xsec_sum += xsec;
     }
     double xsec_avg = xsec_sum / nnuc;
     delete vg;
     return xsec_avg;
   }else{
     return fXSecIntegrator->Integrate(this,in);
   }
 }

void LwlynSmithQELCCPXSec::LoadConfig ( void )

private

Definition at line 414 of file LwlynSmithQELCCPXSec.cxx.

 {
   // Cross section scaling factor
   GetParamDef( "QEL-CC-XSecScale", fXSecScale, 1. ) ;
 
   double thc ;
   GetParam( "CabibboAngle", thc ) ;
   fCos8c2 = TMath::Power(TMath::Cos(thc), 2);
 
    // load QEL form factors model
   fFormFactorsModel = dynamic_cast<const QELFormFactorsModelI *> (
                                              this->SubAlg("FormFactorsAlg"));
   assert(fFormFactorsModel);
   fFormFactors.SetModel(fFormFactorsModel); // <-- attach algorithm
 
    // load XSec Integrator
   fXSecIntegrator =
       dynamic_cast<const XSecIntegratorI *> (this->SubAlg("XSec-Integrator"));
   assert(fXSecIntegrator);
 
   // Get nuclear model for use in Integral()
   RgKey nuclkey = "IntegralNuclearModel";
   fNuclModel = dynamic_cast<const NuclearModelI *> (this->SubAlg(nuclkey));
   assert(fNuclModel);
 
   fLFG = fNuclModel->ModelType(Target()) == kNucmLocalFermiGas;
 
   bool average_over_nuc_mom ;
   GetParamDef( "IntegralAverageOverNucleonMomentum", average_over_nuc_mom, false ) ;
   // Always average over initial nucleons if the nuclear model is LFG
   fDoAvgOverNucleonMomentum = fLFG || average_over_nuc_mom ;
 
   fEnergyCutOff = 0.;
 
   // Get averaging cutoff energy
   GetParamDef("IntegralNuclearInfluenceCutoffEnergy", fEnergyCutOff, 2.0 ) ;
 
   // Method to use to calculate the binding energy of the initial hit nucleon when
   // generating splines
   std::string temp_binding_mode;
   GetParamDef( "IntegralNucleonBindingMode", temp_binding_mode, std::string("UseNuclearModel") );
   fIntegralNucleonBindingMode = genie::utils::StringToQELBindingMode( temp_binding_mode );
 
   // Get PauliBlocker for possible use in FullDifferentialXSec()
   GetParamDef( "IntegralNucleonBindingMode", temp_binding_mode, std::string("UseNuclearModel") );
   fPauliBlocker = dynamic_cast<const PauliBlocker*>( this->SubAlg("PauliBlockerAlg") );
   assert( fPauliBlocker );
 
   // Decide whether or not it should be used in FullDifferentialXSec
   GetParamDef( "DoPauliBlocking", fDoPauliBlocking, true );
 }

bool LwlynSmithQELCCPXSec::ValidProcess ( const Interaction * i ) const

virtual

Can this cross section algorithm handle the input process?

Implements genie::XSecAlgorithmI.

Definition at line 379 of file LwlynSmithQELCCPXSec.cxx.

 {
   if(interaction->TestBit(kISkipProcessChk)) return true;
 
   const InitialState & init_state = interaction->InitState();
   const ProcessInfo &  proc_info  = interaction->ProcInfo();
 
   if(!proc_info.IsQuasiElastic()) return false;
 
   int  nuc = init_state.Tgt().HitNucPdg();
   int  nu  = init_state.ProbePdg();
 
   bool isP   = pdg::IsProton(nuc);
   bool isN   = pdg::IsNeutron(nuc);
   bool isnu  = pdg::IsNeutrino(nu);
   bool isnub = pdg::IsAntiNeutrino(nu);
 
   bool prcok = proc_info.IsWeakCC() && ((isP&&isnub) || (isN&&isnu));
   if(!prcok) return false;
 
   return true;
 }

double LwlynSmithQELCCPXSec::XSec	(	const Interaction *	i,
		KinePhaseSpace_t	k
	)		const

virtual

Compute the cross section for the input interaction.

Implements genie::XSecAlgorithmI.

Definition at line 58 of file LwlynSmithQELCCPXSec.cxx.

 {
   if(! this -> ValidProcess    (interaction) ) {LOG("LwlynSmith",pWARN) << "not a valid process"; return 0.;}
   if(! this -> ValidKinematics (interaction) ) {LOG("LwlynSmith",pWARN) << "not valid kinematics"; return 0.;}
 
   // If computing the full differential cross section, then all four momentum
   // four-vectors (probe, hit nucleon, final lepton, and final nucleon) should
   // have been set already, with the hit nucleon off-shell as appropriate.
   if (kps == kPSQELEvGen) {
     return this->FullDifferentialXSec(interaction);
   }
 
   // Get kinematics & init-state parameters
   const Kinematics &   kinematics = interaction -> Kine();
   const InitialState & init_state = interaction -> InitState();
   const Target & target = init_state.Tgt();
 
   double E  = init_state.ProbeE(kRfHitNucRest);
   double E2 = TMath::Power(E,2);
   double ml = interaction->FSPrimLepton()->Mass();
   double M  = target.HitNucMass();
   double q2 = kinematics.q2();
 
   // One of the xsec terms changes sign for antineutrinos
   bool is_neutrino = pdg::IsNeutrino(init_state.ProbePdg());
   int sign = (is_neutrino) ? -1 : 1;
 
   // Calculate the QEL form factors
   fFormFactors.Calculate(interaction);
 
   double F1V   = fFormFactors.F1V();
   double xiF2V = fFormFactors.xiF2V();
   double FA    = fFormFactors.FA();
   double Fp    = fFormFactors.Fp();
 
 #ifdef __GENIE_LOW_LEVEL_MESG_ENABLED__
   LOG("LwlynSmith", pDEBUG) << "\n" << fFormFactors;
 #endif
 
   // Calculate auxiliary parameters
   double ml2     = TMath::Power(ml,    2);
   double M2      = TMath::Power(M,     2);
   double M4      = TMath::Power(M2,    2);
   double FA2     = TMath::Power(FA,    2);
   double Fp2     = TMath::Power(Fp,    2);
   double F1V2    = TMath::Power(F1V,   2);
   double xiF2V2  = TMath::Power(xiF2V, 2);
   double Gfactor = M2*kGF2*fCos8c2 / (8*kPi*E2);
   double s_u     = 4*E*M + q2 - ml2;
   double q2_M2   = q2/M2;
 
   // Compute free nucleon differential cross section
   double A = (0.25*(ml2-q2)/M2) * (
               (4-q2_M2)*FA2 - (4+q2_M2)*F1V2 - q2_M2*xiF2V2*(1+0.25*q2_M2)
               -4*q2_M2*F1V*xiF2V - (ml2/M2)*(
                (F1V2+xiF2V2+2*F1V*xiF2V)+(FA2+4*Fp2+4*FA*Fp)+(q2_M2-4)*Fp2));
   double B = -1 * q2_M2 * FA*(F1V+xiF2V);
   double C = 0.25*(FA2 + F1V2 - 0.25*q2_M2*xiF2V2);
 
   double xsec = Gfactor * (A + sign*B*s_u/M2 + C*s_u*s_u/M4);
 
   // Apply given scaling factor
   xsec *= fXSecScale;
 
 #ifdef __GENIE_LOW_LEVEL_MESG_ENABLED__
   LOG("LwlynSmith", pDEBUG)
      << "dXSec[QEL]/dQ2 [FreeN](E = "<< E << ", Q2 = "<< -q2 << ") = "<< xsec;
   LOG("LwlynSmith", pDEBUG)
                  << "A(Q2) = " << A << ", B(Q2) = " << B << ", C(Q2) = " << C;
 #endif
 
   //----- The algorithm computes dxsec/dQ2
   //      Check whether variable tranformation is needed
   if(kps!=kPSQ2fE) {
     double J = utils::kinematics::Jacobian(interaction,kPSQ2fE,kps);
 
 #ifdef __GENIE_LOW_LEVEL_MESG_ENABLED__
     LOG("LwlynSmith", pDEBUG)
      << "Jacobian for transformation to: "
                   << KinePhaseSpace::AsString(kps) << ", J = " << J;
 #endif
     xsec *= J;
   }
 
   //----- if requested return the free nucleon xsec even for input nuclear tgt
   if( interaction->TestBit(kIAssumeFreeNucleon) ) return xsec;
 
   //----- compute nuclear suppression factor
   //      (R(Q2) is adapted from NeuGEN - see comments therein)
   double R = nuclear::NuclQELXSecSuppression("Default", 0.5, interaction);
 
   //----- number of scattering centers in the target
   int nucpdgc = target.HitNucPdg();
   int NNucl = (pdg::IsProton(nucpdgc)) ? target.Z() : target.N();
 
 #ifdef __GENIE_LOW_LEVEL_MESG_ENABLED__
   LOG("LwlynSmith", pDEBUG)
        << "Nuclear suppression factor R(Q2) = " << R << ", NNucl = " << NNucl;
 #endif
 
   xsec *= (R*NNucl); // nuclear xsec
 
   return xsec;
 }

Member Data Documentation

double genie::LwlynSmithQELCCPXSec::fCos8c2

private

cos^2(cabibbo angle)

Definition at line 62 of file LwlynSmithQELCCPXSec.h.

bool genie::LwlynSmithQELCCPXSec::fDoAvgOverNucleonMomentum

private

Average cross section over hit nucleon monentum?

Definition at line 69 of file LwlynSmithQELCCPXSec.h.

bool genie::LwlynSmithQELCCPXSec::fDoPauliBlocking

private

Whether to apply Pauli blocking in FullDifferentialXSec.

Definition at line 78 of file LwlynSmithQELCCPXSec.h.

double genie::LwlynSmithQELCCPXSec::fEnergyCutOff

private

Average only for energies below this cutoff defining the region where nuclear modeling details do matter

Definition at line 70 of file LwlynSmithQELCCPXSec.h.

QELFormFactors genie::LwlynSmithQELCCPXSec::fFormFactors

mutableprivate

Definition at line 59 of file LwlynSmithQELCCPXSec.h.

const QELFormFactorsModelI* genie::LwlynSmithQELCCPXSec::fFormFactorsModel

private

Definition at line 60 of file LwlynSmithQELCCPXSec.h.

QELEvGen_BindingMode_t genie::LwlynSmithQELCCPXSec::fIntegralNucleonBindingMode

private

Enum specifying the method to use when calculating the binding energy of the initial hit nucleon during spline generation

Definition at line 75 of file LwlynSmithQELCCPXSec.h.

bool genie::LwlynSmithQELCCPXSec::fLFG

private

If the nuclear model is lfg alway average over nucleons.

Definition at line 68 of file LwlynSmithQELCCPXSec.h.

const NuclearModelI* genie::LwlynSmithQELCCPXSec::fNuclModel

private

Definition at line 67 of file LwlynSmithQELCCPXSec.h.

const genie::PauliBlocker* genie::LwlynSmithQELCCPXSec::fPauliBlocker

private

The PauliBlocker instance to use to apply that correction.

Definition at line 80 of file LwlynSmithQELCCPXSec.h.

const XSecIntegratorI* genie::LwlynSmithQELCCPXSec::fXSecIntegrator

private

Definition at line 61 of file LwlynSmithQELCCPXSec.h.

double genie::LwlynSmithQELCCPXSec::fXSecScale

private

external xsec scaling factor

Definition at line 64 of file LwlynSmithQELCCPXSec.h.

The documentation for this class was generated from the following files:

Generator/src/Physics/QuasiElastic/XSection/LwlynSmithQELCCPXSec.h
Generator/src/Physics/QuasiElastic/XSection/LwlynSmithQELCCPXSec.cxx

Public Member Functions

Private Member Functions

Private Attributes

Additional Inherited Members

Detailed Description

Constructor & Destructor Documentation

Member Function Documentation

Member Data Documentation