module vanilla_interface use types; use consts_dp use pdf_tabulate use convolution; use pdf_general; use dglap_objects use dglap_holders; use pdf_general; use dglap_choices use qcd_coupling use qcd, only: quark_masses_def implicit none !! holds information about the grid type(grid_def), save :: grid, gdarray(4) !! holds the splitting functions type(dglap_holder), save :: dh !! 0 is main pdf table, while i=1:3 contain convolutions with the !! i-loop splitting function type(pdf_table), save :: tables(0:3) logical, save :: setup_done(0:3) = .false. integer, save :: setup_nf(3) = 0 !! coupling logical, save :: coupling_initialised = .false. type(running_coupling), save :: coupling integer, save :: ffn_nf = -1 real(dp), save :: masses(4:6) = quark_masses_def(4:6) end module vanilla_interface !====================================================================== !! initialise the underlying grid, splitting functions and pdf-table !! objects, using the dy and nloop parameters as explained below. subroutine hoppetStart(dy,nloop) use vanilla_interface implicit none !-------------------------------------- real(dp), intent(in) :: dy !! internal grid spacing: 0.1 is a sensible value integer, intent(in) :: nloop !! the maximum number of loops we'll want (<=3) !-------------------------------------- real(dp) :: ymax, Qmin, Qmax, dlnlnQ integer :: order ymax = 12.0d0 Qmin = 1.0d0 Qmax = 28000d0 ! twice LHC c.o.m. dlnlnQ = dy/4.0_dp ! min(0.5_dp*dy,0.07_dp) order = -6 call hoppetStartExtended(ymax,dy,Qmin,Qmax,dlnlnQ,nloop,order,factscheme_MSbar) end subroutine hoppetStart !====================================================================== !! initialise the underlying grid, splitting functions and pdf-table !! objects, using an extended set of parameters, as described below subroutine hoppetStartExtended(ymax,dy,Qmin,Qmax,dlnlnQ,nloop,order,factscheme) use vanilla_interface implicit none real(dp), intent(in) :: ymax !! highest value of ln1/x user wants to access real(dp), intent(in) :: dy !! internal grid spacing: 0.1 is a sensible value real(dp), intent(in) :: Qmin, Qmax !! range in Q real(dp), intent(in) :: dlnlnQ !! internal table spacing in lnlnQ integer, intent(in) :: nloop !! the maximum number of loops we'll want (<=3) integer, intent(in) :: order !! order of numerical interpolation (+ve v. -ve: see below) integer, intent(in) :: factscheme !! 1=unpol-MSbar, 2=unpol-DIS, 3=Pol-MSbar !------------------------------------- ! initialise our grids ! the internal interpolation order (with a minus sign allows ! interpolation to take fake zero points beyond x=1 -- convolution ! times are unchanged, initialisation time is much reduced and ! accuracy is slightly reduced) !order = -5 ! Now create a nested grid call InitGridDef(gdarray(4),dy/27.0_dp,0.2_dp, order=order) call InitGridDef(gdarray(3),dy/9.0_dp,0.5_dp, order=order) call InitGridDef(gdarray(2),dy/3.0_dp,2.0_dp, order=order) call InitGridDef(gdarray(1),dy, ymax ,order=order) call InitGridDef(grid,gdarray(1:4),locked=.true.) ! create the tables that will contain our copy of the user's pdf ! as well as the convolutions with the pdf. call AllocPdfTable(grid, tables(:), Qmin, Qmax, & & dlnlnQ = dlnlnQ, freeze_at_Qmin=.true.) ! initialise splitting-function holder call InitDglapHolder(grid,dh,factscheme=factscheme,& & nloop=nloop,nflo=3,nfhi=6) ! choose a sensible default number of flavours. call SetNfDglapHolder(dh,nflcl=5) ! indicate the pdfs and convolutions have not been initialised... setup_done = .false. end subroutine hoppetStartExtended !====================================================================== !! Given a pdf_subroutine with the interface shown below, initialise !! our internal pdf table. subroutine hoppetAssign(pdf_subroutine) use vanilla_interface ! this module which provides access to the array of tables implicit none interface ! indicate what "interface" pdf_subroutine is expected to have subroutine pdf_subroutine(x,Q,res) use types; implicit none real(dp), intent(in) :: x,Q real(dp), intent(out) :: res(*) end subroutine pdf_subroutine end interface !----------------------------------- ! set up table(0) by copying the values returned by pdf_subroutine onto ! the x-Q grid in table(0) call FillPdfTable_LHAPDF(tables(0), pdf_subroutine) ! indicate that table(0) has been set up setup_done(0) = .true. ! indicate that table(1), table(2), etc... (which will contain the ! convolutions with splitting matrices) have yet to be set up [they ! get set up "on demand" later]. setup_done(1:) = .false. end subroutine hoppetAssign !====================================================================== !! Given a pdf_subroutine with the interface shown below, fill the !! table by evolving the PDF from scale Q0pdf, with alphas provided !! at scale Q0alphas subroutine hoppetEvolve(asQ0, Q0alphas, nloop, muR_Q, pdf_subroutine, Q0pdf) use vanilla_interface ! this module which provides access to the array of tables implicit none implicit none real(dp), intent(in) :: asQ0, Q0alphas, muR_Q, Q0pdf integer, intent(in) :: nloop interface ! indicate what "interface" pdf_subroutine is expected to have subroutine pdf_subroutine(x,Q,res) use types; implicit none real(dp), intent(in) :: x,Q real(dp), intent(out) :: res(*) end subroutine pdf_subroutine end interface !! hold the initial pdf real(dp), pointer :: pdf0(:,:) ! create our internal pdf object for the initial condition call AllocPDF(grid, pdf0) call InitPDF_LHAPDF(grid, pdf0, pdf_subroutine, Q0pdf) ! get a running coupling with the desired scale if (coupling_initialised) call Delete(coupling) if (ffn_nf > 0) then call InitRunningCoupling(coupling, alfas=asQ0, Q=Q0alphas, nloop=nloop, & & fixnf=ffn_nf) else call InitRunningCoupling(coupling, alfas=asQ0, Q=Q0alphas, nloop=nloop, & & quark_masses=masses) end if call AddNfInfoToPdfTable(tables,coupling) coupling_initialised = .true. ! create the tabulation call EvolvePdfTable(tables(0), Q0pdf, pdf0, dh, muR_Q=muR_Q, & & coupling=coupling, nloop=nloop) ! indicate that table(0) has been set up setup_done(0) = .true. ! indicate that table(1), table(2), etc... (which will contain the ! convolutions with splitting matrices) have yet to be set up [they ! get set up "on demand" later]. setup_done(1:) = .false. ! clean up call Delete(pdf0) end subroutine hoppetEvolve !====================================================================== !! Prepare a cached evolution subroutine hoppetPreEvolve(asQ0, Q0alphas, nloop, muR_Q, Q0pdf) use vanilla_interface implicit none real(dp), intent(in) :: asQ0, Q0alphas, muR_Q, Q0pdf integer, intent(in) :: nloop ! get a running coupling with the desired scale if (coupling_initialised) call Delete(coupling) if (ffn_nf > 0) then call InitRunningCoupling(coupling, alfas=asQ0, Q=Q0alphas, nloop=nloop, & & fixnf=ffn_nf) else call InitRunningCoupling(coupling, alfas=asQ0, Q=Q0alphas, nloop=nloop, & & quark_masses=masses) end if call AddNfInfoToPdfTable(tables,coupling) coupling_initialised = .true. ! create the tabulation call PreEvolvePdfTable(tables(0), Q0pdf, dh, muR_Q=muR_Q, & & coupling=coupling, nloop=nloop) end subroutine hoppetPreEvolve !====================================================================== !! Carry out a cached evolution based on the initial condition !! that can be obtained from pdf_subroutine at the scale Q0pdf set in !! PreEvolve subroutine hoppetCachedEvolve(pdf_subroutine) use vanilla_interface implicit none interface ! indicate what "interface" pdf_subroutine is expected to have subroutine pdf_subroutine(x,Q,res) use types; implicit none real(dp), intent(in) :: x,Q real(dp), intent(out) :: res(*) end subroutine pdf_subroutine end interface !! hold the initial pdf real(dp), pointer :: pdf0(:,:) ! create our internal pdf object for the initial condition call AllocPDF(grid, pdf0) call InitPDF_LHAPDF(grid, pdf0, pdf_subroutine, tables(0)%StartScale) ! create the tabulation call EvolvePdfTable(tables(0), pdf0) ! indicate that table(0) has been set up setup_done(0) = .true. ! indicate that table(1), table(2), etc... (which will contain the ! convolutions with splitting matrices) have yet to be set up [they ! get set up "on demand" later]. setup_done(1:) = .false. ! clean up call Delete(pdf0) end subroutine hoppetCachedEvolve !====================================================================== !! Return the coupling at scale Q function hoppetAlphaS(Q) use vanilla_interface ! this module which provides access to the array of tables implicit none real(dp) :: hoppetAlphaS real(dp), intent(in) :: Q hoppetAlphaS = Value(coupling, Q) end function hoppetAlphaS !====================================================================== !! Set up things to be a fixed-flavour number scheme with the given !! fixed_nf number of flavours subroutine hoppetSetFFN(fixed_nf) use vanilla_interface ! this module which provides access to the array of tables implicit none integer, intent(in) :: fixed_nf ffn_nf = fixed_nf end subroutine hoppetSetFFN !====================================================================== !! Set up things to be a variable-flavour number scheme with the given !! quark masses subroutine hoppetSetVFN(mc,mb,mt) use vanilla_interface ! this module which provides access to the array of tables implicit none real(dp) :: mc, mb, mt ffn_nf = -1 masses = (/mc,mb,mt/) end subroutine hoppetSetVFN !====================================================================== !! Return in f(-6:6) the value of the internally stored pdf at the !! given x,Q, with the usual LHApdf meanings for the indices -6:6. subroutine hoppetEval(x,Q,f) use vanilla_interface implicit none real(dp), intent(in) :: x, Q real(dp), intent(out) :: f(-6:6) call EvalPdfTable_xQ(tables(0),x,Q,f) end subroutine hoppetEval !====================================================================== !! Return in f(-6:6) the value of !! !! [P(iloop,nf) \otimes pdf] (x,Q) !! !! where P(iloop,nf) is the iloop-splitting function for the given !! value of nf, and pdf is our internally stored pdf. !! !! The normalisation is such that the nloop dglap evolution equation is !! !! dpdf/dlnQ^2 = sum_{iloop=1}^nloop !! (alphas/(2*pi))^iloop * P(iloop,nf) \otimes pdf !! !! Note that each time nf changes relative to a previous call for the !! same iloop, the convolution has to be repeated for the whole !! table. So for efficient results when requiring multiple nf values, !! calls with the same nf value should be grouped together. !! !! In particular, for repeated calls with the same value of nf, the !! convolutions are carried out only on the first call (i.e. once for !! each value of iloop). Multiple calls with different values for !! iloop can be carried out without problems. !! subroutine hoppetEvalSplit(x,Q,iloop,nf,f) use vanilla_interface; use warnings_and_errors implicit none real(dp), intent(in) :: x, Q integer, intent(in) :: iloop, nf real(dp), intent(out) :: f(-6:6) integer :: iQ if (.not. setup_done(iloop) .or. setup_nf(iloop) /= nf) then if (iloop > size(dh%allP,dim=1) .or. iloop < 1) & &call wae_error('hoppetEvalSplit','illegal value for iloop:',& &intval=iloop) if (nf < 0) then ! use whatever nf is relevant if (.not. tables(0)%nf_info_associated) call wae_error(& & 'hoppetEvalSplit','automatic choice of nf (nf<0) but the tabulation has no information on nf') do iQ = 0, tables(0)%nQ tables(iloop)%tab(:,:,iQ) = dh%allP(iloop, tables(0)%nf_int(iQ)) & & .conv. tables(0)%tab(:,:,iQ) end do else ! use a fixed nf if (nf < lbound(dh%allP,dim=2) .or. nf > ubound(dh%allP,dim=2)) & &call wae_error('hoppetEvalSplit','illegal value for nf:',& &intval=nf) tables(iloop)%tab = dh%allP(iloop, nf) .conv. tables(0)%tab end if setup_done(iloop) = .true. setup_nf(iloop) = nf end if call EvalPdfTable_xQ(tables(iloop),x,Q,f) end subroutine hoppetEvalSplit