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/lepton2p2h [ Modules ]

[ Top ] [ Modules ]

NAME

module lepton2p2h

PURPOSE

Do all the internals for 2p2h scattering:

EM:

  • ell N1 N2 --> ell' N1' N2' == gamma* N1 N2 --> N1' N2'
  • ell N1 N2 --> ell' N Delta == gamma* N1 N2 --> N Delta

NC:

  • nu N1 N2 --> nu' N1' N2'
  • nu N1 N2 --> nu' N Delta

CC:

  • nu N1 N2 --> ell- N1' N2' (sum of hadronic charges increases by +1)
  • nu N1 N2 --> ell- N Delta ( -- " -- )

antiEM, antiNC and antiCC are the same as EM, NC, CC.


lepton2p2h/ME_Version [ Global module-variables ]

[ Top ] [ lepton2p2h ] [ Global module-variables ]

PURPOSE

indicate the type of matrix element parametrisation

SOURCE

  integer, save :: ME_Version = 8
  !
  ! possible values:
  ! * 1: Monopole parametrisation (cf. const*ME_Norm_XX/(1+ Q^2/ME_Mass_XX^2)^2 ) ! const for CC  fitted to MiniBooNE is 3.5e-6
  ! * 2: Monopole parameterization in transverse part only ! const for CC  fitted to MiniBooNE is 1e-4
  ! * 3: Monopole with suppressed low Q2  ( ME_Norm_XX*Q2/(1+ Q^2/ME_Mass_XX^2)^2 )
  ! * 4: const ME_Norm_XX  ! const for CC  fitted to MiniBooNE is 1.8e-6
  ! * 5: const with transverse part only
  ! * 6: fall with W
  ! * 7: as 4  and decreasing with Enu
  ! * 8: as 5  and decreasing with Enu
  ! * 9: exponential fall with Q2
  ! * 10: transverse,  exponential fall with Q2
  ! * 11:
  ! * 12: "Dipole transverse" transverse,  fall with Q2 as 4-th power
  ! * 13: transverse,  fall with Enu
  ! * 14: transverse,  fall with qz^2
  ! * 15: like Bosted arXiV:1203.2262  and transverse

lepton2p2h/ME_Norm_QE [ Global module-variables ]

[ Top ] [ lepton2p2h ] [ Global module-variables ]

PURPOSE

Parametrisation of matrix element, parameter no. 1,

for (EM,CC,NC)

SOURCE

  real,dimension(1:3), save :: ME_Norm_QE    = (/1.0, 1.0, 1.0/)

NOTES

The value == 1 is a dummy value


lepton2p2h/ME_Norm_Delta [ Global module-variables ]

[ Top ] [ lepton2p2h ] [ Global module-variables ]

PURPOSE

Parametrisation of matrix element, parameter no. 1,

for (EM,CC,NC)

SOURCE

  real,dimension(1:3), save :: ME_Norm_Delta = (/1.0, 1.0, 1.0/)

NOTES

The value == 1 is a dummy value


lepton2p2h/ME_Mass_QE [ Global module-variables ]

[ Top ] [ lepton2p2h ] [ Global module-variables ]

PURPOSE

Parametrisation of matrix element, parameter no. 2

for (EM,CC,NC)

SOURCE

  real,dimension(1:3), save :: ME_Mass_QE    = (/1.0, 1.0, 1.0/)

NOTES

The value == 1 is a dummy value


lepton2p2h/ME_Mass_Delta [ Global module-variables ]

[ Top ] [ lepton2p2h ] [ Global module-variables ]

PURPOSE

Parametrisation of matrix element, parameter no. 2

for (EM,CC,NC)

SOURCE

  real,dimension(1:3), save :: ME_Mass_Delta = (/1.0, 1.0, 1.0/)

NOTES

The value == 1 is a dummy value


lepton2p2h/readInput [ Subroutines ]

[ Top ] [ lepton2p2h ] [ Subroutines ]

NAME

subroutine readInput


lepton2p2h/Lepton2p2h [ Namelists ]

[ Top ] [ lepton2p2h ] [ Namelists ]

NAME

NAMELIST /Lepton2p2h/

PURPOSE

Includes parameters for QE events:


lepton2p2h/lepton2p2h_SelectN2 [ Subroutines ]

[ Top ] [ lepton2p2h ] [ Subroutines ]

NAME

subroutine lepton2p2h_SelectN2(eN)

PURPOSE

Finds the second nucleon for the 2p2h collision

INPUTS

OUTPUT

NOTES

  • The seond particle is generated analytically, not by selecting a testparticle from the real particle vector.
  • This is at a very basic level. You may add more sophisticated features as eq. two-particle correlatione etc.
  • A threshold check Wfree>(2*mN+1MeV) is performed


lepton2p2h/lepton2p2h_XS [ Functions ]

[ Top ] [ lepton2p2h ] [ Functions ]

NAME

real function lepton2p2h_XS(eN,outPart,DoQE)

PURPOSE

calculate the electron induced 2p2h-QE cross section

INPUTS

  • type(electronNucleon_event) :: eN -- electron-Nucleon event info
  • type(particle),dimension(:) :: OutPart -- the outgoing particles
  • logical :: DoQE -- .true. for NN final state, .false. for N Delta

OUTPUT

  • the function value

NOTES

  • One has to give a realistic parametrization of the matrix element
  • If one randomly selects the position of the second particle, one has to respect this in the XS calculation (and maybe not to multiply it with the density at the position)


lepton2p2h_XS/ME_Monopole [ Functions ]

[ Top ] [ lepton2p2h_XS ] [ Functions ]

NAME

real function ME_Monopole(eN)

PURPOSE

calculate the matrix element according the monopole parametrisation of the "form factor" so that the ME falls down as dipole


lepton2p2h_XS/ME_Monopole_transverse [ Functions ]

[ Top ] [ lepton2p2h_XS ] [ Functions ]

NAME

real function ME_dipole_transverse(eN)

PURPOSE

calculate the 2p2h matrix element according to W_1(g_munu -q_um q_nu /Q2) * L^munu so that the contribution is only to the transverse part

NOTES

You have full access to all incoming and outgoing particles:

  • eN%lepton_in -- incoming lepton
  • eN%nucleon -- incoming nucleon 1
  • eN%nucleon2 -- incoming nucleon 2

exchanged boson:

  • eN%boson -- exchanged boson

even without considering the final state particles, you know the kind of process via 'eN%idProcess', which may take the values EM,NC,CC and also antiEM,antiNC,antiCC


lepton2p2h_XS/ME_Dipole [ Functions ]

[ Top ] [ lepton2p2h_XS ] [ Functions ]

NAME

real function ME_Dipole(eN)

PURPOSE

calculate the 2p2h matrix element according the dipole parametrisation


lepton2p2h_XS/ME_Dipole_transverse [ Functions ]

[ Top ] [ lepton2p2h_XS ] [ Functions ]

NAME

real function ME_Dipole_transverse(eN)

PURPOSE

calculate the 2p2h matrix element according to W_1(g_munu -q_um q_nu /Q2) * L^munu so that the contribution is only to the transverse part

NOTES

You have full access to all incoming and outgoing particles:

  • eN%lepton_in -- incoming lepton
  • eN%nucleon -- incoming nucleon 1
  • eN%nucleon2 -- incoming nucleon 2

exchanged boson:

  • eN%boson -- exchanged boson

even without considering the final state particles, you know the kind of process via 'eN%idProcess', which may take the values EM,NC,CC and also antiEM,antiNC,antiCC


lepton2p2h_XS/ME_von_qz2_transverse [ Functions ]

[ Top ] [ lepton2p2h_XS ] [ Functions ]

NAME

real function ME_von_qz2_transverse(eN)

PURPOSE

calculate the 2p2h matrix element according to W_1(g_munu -q_um q_nu /Q2) * L^munu so that the contribution is only to the transverse part

NOTES

You have full access to all incoming and outgoing particles:

  • eN%lepton_in -- incoming lepton
  • eN%nucleon -- incoming nucleon 1
  • eN%nucleon2 -- incoming nucleon 2

exchanged boson:

  • eN%boson -- exchanged boson

even without considering the final state particles, you know the kind of process via 'eN%idProcess', which may take the values EM,NC,CC and also antiEM,antiNC,antiCC


lepton2p2h_XS/ME_Bosted_transverse [ Functions ]

[ Top ] [ lepton2p2h_XS ] [ Functions ]

NAME

real function ME_Bosted_transverse(eN)

PURPOSE

calculate the 2p2h matrix element according to W_1(g_munu -q_um q_nu /Q2) * L^munu so that the contribution is only to the transverse part W1 is taken from Bosted, Mamyan arXiv:1303.2262

NOTES

You have full access to all incoming and outgoing particles:

  • eN%lepton_in -- incoming lepton
  • eN%nucleon -- incoming nucleon 1
  • eN%nucleon2 -- incoming nucleon 2

exchanged boson:

  • eN%boson -- exchanged boson

even without considering the final state particles, you know the kind of process via 'eN%idProcess', which may take the values EM,NC,CC and also antiEM,antiNC,antiCC


lepton2p2h/lepton2p2h_FinalState [ Subroutines ]

[ Top ] [ lepton2p2h ] [ Subroutines ]

NAME

subroutine lepton2p2h_FinalState(eN,outPart,DoQE,flagOK)

PURPOSE

Generate the final state of the electron 2p2h event


lepton2p2h/lepton2p2h_DoQE [ Subroutines ]

[ Top ] [ lepton2p2h ] [ Subroutines ]

NAME

subroutine lepton2p2h_DoQE(eN,outPart,XS)

PURPOSE

Do all the electron induced 2p2h-QE scattering gamma* N1 N2 -> N1' N2'

INPUTS

OUTPUT

  • type(particle), dimension(:) :: OutPart -- the two produced nucleons
  • real :: XS -- the cross section


lepton2p2h/lepton2p2h_DoDelta [ Subroutines ]

[ Top ] [ lepton2p2h ] [ Subroutines ]

NAME

subroutine lepton2p2h_DoDelta(eN,outPart,XS)

PURPOSE

Do all the electron induced 2p2h-QE scattering gamma* N1 N2 -> N Delta

INPUTS

OUTPUT

  • type(particle), dimension(:) :: OutPart -- the two produced hadrons
  • real :: XS -- the cross section