Namespace List

Here is a list of all namespaces with brief descriptions:

[detail level 123]

►Napfel	Namespace for all APFEL++ functions and classes
CAlphaQCD	The AlphaQCD is a specialization class of the MatchedEvolution class for the computation of the QCD coupling running
CAlphaQCDg	The AlphaQCDg is a specialization class of the MatchedEvolution class for the computation of the QCD coupling running using the analytic g functions
CAlphaQCDQED	The AlphaQCDQED is a specialization class of the MatchedEvolution class for the computation of the mixed evolution of QCD and QED
CAlphaQCDxi	The AlphaQCDxi is a specialization class of the MatchedEvolution class for the computation of the QCD coupling running with the possibility to vary the resummation scale through the parameter xi
CAlphaQED	The AlphaQED is a specialization class of the MatchedEvolution class for the computation of the QED coupling running
CANS2qqH_0	O(αs2) constant term of eq (B.4) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CANS2qqH_L	O(αs2) term propotional to ln(μ2/m2) of eq (B.4) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CANS2qqH_L2	O(αs2) term propotional to ln2(μ2/m2) of eq (B.4) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CANS3qqH_0	O(αs3) constant term
CAPS2Hq_0	O(αs2) constant term of eq (B.1) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAPS2Hq_L	O(αs2) term propotional to ln(μ2/m2) of eq (B.1) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAPS2Hq_L2	O(αs2) term propotional to ln2(μ2/m2) of eq (B.1) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAPS3Hq_0	O(αs3) constant term
CAS1ggH_L	O(αs) term propotional to ln(μ2/m2) of eq (B.6) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS1gH_0	O(αs) constant term for the gH matching. This is the QCD adaptation of Eq. (4.189) of https://arxiv.org/pdf/1909.03886.pdf
CAS1gH_L	O(αs) term propotional to ln(μ2/m2) for the gH matching. This is the QCD adaptation of Eq. (4.189) of https://arxiv.org/pdf/1909.03886.pdf
CAS1Hg_L	O(αs) term propotional to ln(μ2/m2) of eq. (B.2) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS1HH_0	O(αs) constant term for the HH matching. This is the QCD adaptation of Eq. (4.121) of https://arxiv.org/pdf/1909.03886.pdf
CAS1HH_L	O(αs) term propotional to ln(μ2/m2) for the HH matching. This is the QCD adaptation of Eq. (4.121) of https://arxiv.org/pdf/1909.03886.pdf
CAS1polggH_L	O(αs) term propotional to ln(μ2/m2)
CAS1polgH_0	O(αs) constant term for the gH matching
CAS1polgH_L	O(αs) term propotional to ln(μ2/m2) for the gH matching
CAS1polHg_L	O(αs) term propotional to ln(μ2/m2)
CAS1polHH_0	O(αs) constant term for the HH matching
CAS1polHH_L	O(αs) term propotional to ln(μ2/m2) for the HH matching
CAS2ggH_0	O(αs2) constant term of eq (B.7) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS2ggH_L	O(αs2) term propotional to ln(μ2/m2) of eq (B.7) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS2ggH_L2	O(αs2) term propotional to ln2(μ2/m2) of eq (B.7) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS2gqH_0	O(αs2) constant term of eq (B.5) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS2gqH_L	O(αs2) term propotional to ln(μ2/m2) of eq (B.5) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS2gqH_L2	O(αs2) term propotional to ln2(μ2/m2) of eq (B.5) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS2Hg_0	O(αs2) constant term of eq (B.3) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS2Hg_L	O(αs2) term propotional to ln(μ2/m2) of eq (B.3) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS2Hg_L2	O(αs2) term propotional to ln2(μ2/m2) of eq (B.3) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CAS3ggH_0	O(αs3) constant term
CAS3gqH_0	O(αs3) constant term
CAS3Hg_0	O(αs3) constant term
CATS1ggH_L	O(αs) term propotional to ln(μ2/m2) of eq. (22) of https://arxiv.org/pdf/hep-ph/0504192.pdf
CATS1gH_L	O(αs) term propotional to ln(μ2/m2) of eq. (B.2) of https://arxiv.org/pdf/hep-ph/9612398.pdf
CATS1Hg_0	O(αs) constant term of eq. (15) of https://arxiv.org/pdf/hep-ph/0504192.pdf
CATS1Hg_L	O(αs) term propotional to ln(μ2/m2) of eq. (15) of https://arxiv.org/pdf/hep-ph/0504192.pdf
CATS1HH_0	O(αs) constant term for the HH matching. This is the QCD adaptation of Eq. (4.121) of https://arxiv.org/pdf/1909.03886.pdf
CATS1HH_L	O(αs) term propotional to ln(μ2/m2) for the HH matching. This is the QCD adaptation of Eq. (4.121) of https://arxiv.org/pdf/1909.03886.pdf
CC1ggff	The O(αs) gluon-gluon matching function for FFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC1ggpdf	The O(αs) gluon-gluon matching function for PDFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC1ggpdfBM	The O(αs) gluon-gluon matching function for linearly polarised gluon PDF (reference: https://arxiv.org/pdf/1907.03780.pdf)
CC1ggpdfg1	The O(αs) gluon-gluon matching function for g1 PDFs (reference: https://arxiv.org/pdf/1702.06558.pdf)
CC1gqff	The O(αs) gluon-quark matching function for FFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC1gqpdf	The O(αs) gluon-quark matching function for PDFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC1gqpdfBM	The O(αs) gluon-quark matching function for linearly polarised gluon PDF (reference: https://arxiv.org/pdf/1907.03780.pdf)
CC1gqpdfg1	The O(αs) gluon-quark matching function for g1 PDFs (reference: https://arxiv.org/pdf/1702.06558.pdf)
CC1nsff	The O(αs) non-singlet matching function for FFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC1nspdf	The O(αs) non-singlet matching function for PDFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC1nspdfg1	The O(αs) non-singlet matching function for g1 PDFs (reference: https://arxiv.org/pdf/1702.06558.pdf)
CC1nspdfSivers	The O(αs) non-singlet matching function for Sivers PDFs (see Eq. (A.9) of https://arxiv.org/pdf/2009.10710.pdf)
CC1qgff	The O(αs) quark-gluon matching function for FFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC1qgpdf	The O(αs) quark-gluon matching function for PDFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC1qgpdfg1	The O(αs) quark-gluon matching function for g1 PDFs (reference: https://arxiv.org/pdf/1702.06558.pdf)
CC21g	O(αs) gluon coefficient function for F2
CC21ns	O(αs) non-singlet coefficient function for F2
CC21Tg	O(αs) gluon coefficient function for F2 in SIA
CC21Tns	O(αs) non-singlet coefficient function for F2 in SIA
CC22g	O(αs2) gluon coefficient function for F2
CC22nsm	O(αs2) non-singlet-minus coefficient function for F2
CC22nsp	O(αs2) non-singlet-plus coefficient function for F2
CC22ps	O(αs2) pure-singlet coefficient function for F2
CC22Tg	O(αs2) gluon coefficient function for F2 in SIA
CC22Tnsp	O(αs2) non-singlet-plus coefficient function for F2 in SIA
CC22Tps	O(αs2) pure-singlet coefficient function for F2 in SIA
CC23g	O(αs3) gluon coefficient function for F2
CC23nsm	O(αs3) non-singlet-minus coefficient function for F2
CC23nsp	O(αs3) non-singlet-plus coefficient function for F2
CC23ps	O(αs3) pure-singlet coefficient function for F2
CC2ggff	The O(αs2) gluon-gluon matching function for FFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC2ggpdf	The O(αs2) gluon-gluon matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC2ggpdfBM	The O(αs2) gluon-gluon matching function for linearly polarised gluon PDFs (reference: https://arxiv.org/pdf/1907.03780.pdf)
CC2gqff	The O(αs2) gluon-quark matching function for FFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC2gqpdf	The O(αs2) gluon-quark matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC2gqpdfBM	The O(αs2) gluon-quark matching function for linearly polarised gluon PDF (reference: https://arxiv.org/pdf/1907.03780.pdf)
CC2nsmff	The O(αs2) quark-antiquark matching function for FFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC2nsmpdf	The O(αs2) valence minus matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC2nspff	The O(αs2) quark-quark matching function for FFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC2nsppdf	The O(αs2) valence plus matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC2psff	The O(αs2) pure-singlet matching function for FFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC2pspdf	The O(αs2) pure-singlet matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC2qgff	The O(αs2) quark-gluon matching function for FFs (references: https://arxiv.org/pdf/1604.07869.pdf and https://arxiv.org/pdf/1706.01473.pdf)
CC2qgpdf	The O(αs2) quark-gluon matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC31ns	O(αs) non-singlet coefficient function for F3
CC31Tns	O(αs) non-singlet coefficient function for F3 in SIA
CC32nsm	O(αs2) non-singlet-minus coefficient function for F3
CC32nsp	O(αs2) non-singlet-plus coefficient function for F3
CC32Tnsp	O(αs2) non-singlet-plus coefficient function for F3 in SIA
CC33nsm	O(αs3) non-singlet-minus coefficient function for F3
CC33nsp	O(αs3) non-singlet-plus coefficient function for F3
CC33nsv	O(αs3) total-valence coefficient function for F3
CC3ggff	The O(αs3) gluon-gluon matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3ggpdf	The O(αs3) gluon-gluon matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3gqff	The O(αs3) gluon-quark matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3gqpdf	The O(αs3) gluon-quark matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3nsmff	The O(αs3) valence minus matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3nsmpdf	The O(αs3) valence minus matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3nspff	The O(αs3) valence plus matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3nsppdf	The O(αs3) valence plus matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3psff	The O(αs3) pure-singlet matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3pspdf	The O(αs3) pure-singlet matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3pvff	The O(αs3) pure-valence matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3pvpdf	The O(αs3) pure-valence matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3qgff	The O(αs3) quark-gluon matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CC3qgpdf	The O(αs3) quark-gluon matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf)
CCgtmd1gg	The O(αs) gluon-gluon unpolarised matching function for GTMDs
CCgtmd1gq	The O(αs) gluon-quark unpolarised matching function for GTMDs
CCgtmd1ns	The O(αs) non-singlet unpolarised matching function for GTMDs
CCgtmd1qg	The O(αs) quark-gluon unpolarised matching function for GTMDs
CCgtmd1qq	The O(αs) quark-quark unpolarised matching function for GTMDs
CCL1g	O(αs) gluon coefficient function for FL
CCL1ns	O(αs) non-singlet coefficient function for FL
CCL1Tg	O(αs) gluon coefficient function for FL in SIA
CCL1Tns	O(αs) non-singlet coefficient function for FL in SIA
CCL2g	O(αs2) gluon coefficient function for FL
CCL2nsm	O(αs2) non-singlet-minus coefficient function for FL
CCL2nsp	O(αs2) non-singlet-plus coefficient function for FL
CCL2ps	O(αs2) pure-singlet coefficient function for FL
CCL2Tg	O(αs2) gluon coefficient function for FL in SIA
CCL2Tnsp	O(αs2) non-singlet-plus coefficient function for FL in SIA
CCL2Tps	O(αs2) pure-singlet coefficient function for FL in SIA
CCL3g	O(αs3) gluon coefficient function for FL
CCL3nsm	O(αs3) non-singlet-minus coefficient function for FL
CCL3nsp	O(αs3) non-singlet-plus coefficient function for FL
CCL3ps	O(αs3) pure-singlet coefficient function for FL
CCm021gNC_c	O(αs) gluon coefficient function for F2. Constant term
CCm021gNC_l	O(αs) gluon coefficient function for F2. Single-log term
CCm022gNC_c	O(αs2) gluon coefficient function for F2. Constant term
CCm022gNC_f	O(αs2) gluon coefficient function for F2. Single-log(μF) term
CCm022gNC_l	O(αs2) gluon coefficient function for F2. Single-log term
CCm022gNC_l2	O(αs2) gluon coefficient function for F2. Double-log term
CCm022gNC_lf	O(αs2) gluon coefficient function for F2. Mixed-double-log term
CCm022nsNC_c	O(αs2) non-singlet coefficient function for F2. Constant term
CCm022nsNC_l	O(αs2) non-singlet coefficient function for F2. Single-log term
CCm022nsNC_l2	O(αs2) non-singlet coefficient function for F2. Double-log term
CCm022psNC_c	O(αs2) pure-singlet coefficient function for F2. Constant term
CCm022psNC_f	O(αs2) pure-singlet coefficient function for F2. Single-log(μF) term
CCm022psNC_l	O(αs2) pure-singlet coefficient function for F2. Single-log term
CCm022psNC_l2	O(αs2) pure-singlet coefficient function for F2. Double-log term
CCm022psNC_lf	O(αs2) pure-singlet coefficient function for F2. Mixed-double-log term
CCm0L1gNC_c	O(αs) gluon coefficient function for FL. Constant term
CCm0L2gNC_c	O(αs2) gluon coefficient function for FL. Constant term
CCm0L2gNC_f	O(αs2) gluon coefficient function for FL. Single-log(μF) term
CCm0L2gNC_l	O(αs2) gluon coefficient function for FL. Single-log term
CCm0L2nsNC_c	O(αs2) non-singlet coefficient function for FL. Constant term
CCm0L2nsNC_l	O(αs2) non-singlet coefficient function for FL. Single-log term
CCm0L2psNC_c	O(αs2) pure-singlet coefficient function for FL. Constant term
CCm0L2psNC_f	O(αs2) pure-singlet coefficient function for FL. Single-log(μF) term
CCm0L2psNC_l	O(αs2) pure-singlet coefficient function for FL. Single-log term
CCm11ns	O(αs) non-singlet coefficient function for 2xF1. The relevant function is in Eq. (C4) of https://arxiv.org/pdf/hep-ph/9805233.pdf
CCm21gCC	O(αs) gluon coefficient function for F2
CCm21gNC	O(αs) gluon coefficient function for F2. See eq. (53) of https://arxiv.org/pdf/1001.2312.pdf. Or it uses the fortran routines in 'src/dis/hqcoef.f'
CCm21ns	O(αs) non-singlet coefficient function for F2. The relevant function is in Eq. (C4) of https://arxiv.org/pdf/hep-ph/9805233.pdf
CCm21qCC	O(αs) quark coefficient function for F2
CCm22bargNC	O(αs2) gluon coefficient function proportional to ln(Q2/M2) for F2. Uses the fortran routines in 'src/dis/hqcoef.f'
CCm22barpsNC	O(αs2) pure-singlet coefficient function proportional to ln(Q2/M2) for F2. Uses the fortran routines in 'src/dis/hqcoef.f'
CCm22gNC	O(αs2) gluon coefficient function for F2. Uses the fortran routines in 'src/dis/hqcoef.f'
CCm22nsNC	O(αs2) non-singlet coefficient function for F2. See Appendix A of https://arxiv.org/pdf/hep-ph/9601302.pdf. Or it uses the fortran routines in 'src/dis/hqcoef.f'
CCm22psNC	O(αs2) pure-singlet coefficient function for F2. Uses the fortran routines in 'src/dis/hqcoef.f'
CCm31gCC	O(αs) gluon coefficient function for xF3
CCm31ns	O(αs) non-singlet coefficient function for F3. The relevant function is in Eq. (C4) of https://arxiv.org/pdf/hep-ph/9805233.pdf
CCm31qCC	O(αs) quark coefficient function for xF3
CCmL1gCC	O(αs) gluon coefficient function for FL
CCmL1gNC	O(αs) gluon coefficient function for FL
CCmL1ns	O(αs) non-singlet coefficient function for FL = F2 - 2xF1. The relevant function is in Eq. (C4) of https://arxiv.org/pdf/hep-ph/9805233.pdf
CCmL1qCC	O(αs) quark coefficient function for FL
CCmL2bargNC	O(αs2) gluon coefficient function proportional to ln(Q2/M2) for FL. Uses the fortran routines in 'src/dis/hqcoef.f'
CCmL2barpsNC	O(αs2) pure-singlet coefficient function proportional to ln(Q2/M2) for FL. Uses the fortran routines in 'src/dis/hqcoef.f'
CCmL2gNC	O(αs2) gluon coefficient function for FL. Uses the fortran routines in 'src/dis/hqcoef.f'
CCmL2nsNC	O(αs2) non-singlet coefficient function for FL. See Appendix A of https://arxiv.org/pdf/hep-ph/9601302.pdf. Or it uses the fortran routines in 'src/dis/hqcoef.f'
CCmL2psNC	O(αs2) pure-singlet coefficient function for FL. Uses the fortran routines in 'src/dis/hqcoef.f'
►CConvolutionMap	Encapsulates the set of rules to multiply a sets of operators with a set of distributions
Crule	This structure contains the attribute of a single rule
CDglap	The Dglap class is specialization class of the MatchedEvolution class for the computation of the DGLAP evolution
CDglapObjects	Structure that contains all the precomputed quantities needed to perform the DGLAP evolution, i.e. perturbative coefficients of splitting functions and matching conditions, and the heavy quark thresholds
CDiagonalBasis	Simplest derivation of ConvolutionMap meant to essentially perform a scalar product of two sets of objects
CDISCCBasis	Derived of ConvolutionMap specialised for the computation of the CC DIS structure functions
CDISNCBasis	Derived of ConvolutionMap specialised for the computation of the NC DIS structure functions
CDistribution	Defines one of the basic objects of APFEL++. This is essentially the discretisation of a function that can be conveniently used for convolutions
CDoubleExponentialQuadrature	DE-Quadrature Numerical automatic integrator for improper integral using double dxponential (DE) quadrature. The code is a manipulation of the code linked here:
CDoubleObject	The DoubleObject class is a collection of pairs of single objects (Distributions or Operators) accompained by a multiplicative constant. This mother class provides the basic ingredients for the computation double convolutions required in SIDIS and DY
CEvolBasisPlusMinus	Derives from ConvolutionMap and implements a basis in which plus (q+qbar) and minus (q-qbar) combinations are fully coupled
CEvolutionBasisQCD	Derived of ConvolutionMap specialised for the DGLAP evolution of distributions using the QCD evolution basis
CEvolutionOperatorBasisQCD	Derived of ConvolutionMap specialised for the DGLAP evolution of operators using the QCD evolution basis
►CEvolutionSetup	The EvolutionSetup structure is a collection of all possible evolution parameters
CGridParameters	Structure for the subgrid parameters
CEvolveDistributionsBasisQCD	Derived of ConvolutionMap specialised to match a set of evolution operators to a set a initial-scale distributions
CExpression	Encapsulates in a proper form a given analytic expression in such a way that it can be transformed into an operator
CExtendedVector	Class that extends vectors to negative indices
CG11g	O(αs) gluon coefficient function for for g1
CG11ns	O(αs) non-singlet coefficient function for g1
CG12g	O(αs2) gluon coefficient function for F2
CG12nsp	O(αs2) non-singlet-plus coefficient function for F2
CG12ps	O(αs2) pure-singlet coefficient function for F2
CG41ns	O(αs) non-singlet coefficient function for g4
CGL1ns	O(αs) non-singlet coefficient function for gL
CGrid	Defines ab object that is essentially a collection of "SubGrid" objects plus other global parameters. This class also includes all the relevant methods for the manipulation of the SubGrids
CGtmdObjects
CIdentity	Derived class from Expression to implement the Identity operator (delta function)
CInitialiseEvolution	The InitialiseEvolution performs all the operations to initialise a DGLAP evolution using an EvolutionSetup object to retrieve the relevant information. This class also provides the necessary functions to access the evolved distributions, coupling(s), and masses
CIntegrator	Performs unidimensional numerical integrations using the Guassian quadrature
CIntegrator2D	Performs two-dimensional numerical integrations using the Guassian quadrature
CInterpolator	Mother class for the x-space interpolationand requires the implementation of a specialized interpolation algorithm. The current version uses the joint grid object stored allocated by the Grid class
CLagrangeInterpolator	Specialization of the Interpolator class using the lagrange interpolation procedure
CLHKnotArray	The LHKnotArray structure emulates the KnotArray1F class of LHAPDF and contains the grids in x, Q2 (only a given subgrid), and one single distribution tabulated on the (x,Q) bidimensional grid
CMatchedEvolution	The MatchedEvolution class is a template mother class for the computation of the running of a generic quantity in a VFNS. It provides the basic ingredients for the computation and the heavy-quark threshold matching of the running of a given object
CMatchingBasisQCD	Derived of ConvolutionMap specialised for the matching of distributions using the QCD evolution basis and without assuming that intrinsic heavy quark contributions vanish
CMatchingOperatorBasisQCD	Derived of ConvolutionMap specialised for the matching of the evolution of operators at the heavy-quark thresholds using the QCD evolution basis
Cmatrix	The matrix class is a simple implementation of 2d arrays based on a continous memory allocation. Elements are accessible throught the (i,j) operator
CNull	Derived class from Expression to implement the Null operator (zero)
►CObservable	The Observable class encapsulates sets of operators and sets of T-type objects for an easy computation of observables deriving from the convolution of the two. This class can contain an arbitrary number of such pairs that are separatately convoluted and joint when the obeservable is computed by means of the "Evaluate" function
CConvolutionPair	This structure contains a pair of sets of coefficient functions and of objects
COgataQuadrature	Implements the Hankel-transform of the input function using the Ogata quadrature method described here: http://www.kurims.kyoto-u.ac.jp/~okamoto/paper/Publ_RIMS_DE/41-4-40.pdf
COperator	Defines the basic object "Operator" which is essentially the convolution on the grid bewteen an Expression object (e.g. a splitting function) and the interpolant functions
CP0gg	Space-like O(αs) gluon-gluon unpolarised splitting function
CP0gq	Space-like O(αs) gluon-quark unpolarised splitting function
CP0ns	Space-like O(αs) non-singlet unpolarised splitting function
CP0polgg	Space-like O(αs) gluon-gluon longitudinally polarised splitting function
CP0polgq	Space-like O(αs) gluon-quark longitudinally polarised splitting function
CP0polns	Space-like O(αs) non-singlet longitudinally polarised splitting function. This is equal to the non-singlet unpolarised splitting function
CP0polqg	Space-like O(αs) quark-gluon longitudinally polarised splitting function
CP0qg	Space-like O(αs) quark-gluon unpolarised splitting function
CP0Tgg	Time-like O(αs) gluon-gluon unpolarised splitting function
CP0Tgq	Time-like O(αs) gluon-quark unpolarised splitting function
CP0Tns	Time-like O(αs) non-singlet unpolarised splitting function
CP0Tqg	Time-like O(αs) quark-gluon unpolarised splitting function
CP0transgg	Space-like O(αs) gluon-gluon linearly polarised splitting function
CP0transns	Space-like O(αs) non-singlet transversely polarised splitting function
CP0Ttransns	Time-like O(αs) non-singlet transversely polarised splitting function
CP1gg	Space-like O(αs2) gluon-gluon unpolarised splitting function
CP1gq	Space-like O(αs2) gluon-quark unpolarised splitting function
CP1nsm	Space-like O(αs2) non-singlet-minus unpolarised splitting function
CP1nsp	Space-like O(αs2) non-singlet-plus unpolarised splitting function
CP1polgg	Space-like O(αs2) gluon-gluon longitudinally polarised splitting function
CP1polgq	Space-like O(αs2) gluon-quark longitudinally polarised splitting function
CP1polnsm	Space-like O(αs2) non-singlet-minus longitudinally polarised splitting function. This is equal to the non-singlet-plus unpolarised splitting function
CP1polnsp	Space-like O(αs2) non-singlet-plus longitudinally polarised splitting function. This is equal to the non-singlet-minus unpolarised splitting function
CP1polps	Space-like O(αs2) pure-singlet longitudinally polarised splitting function
CP1polqg	Space-like O(αs2) quark-gluon longitudinally polarised splitting function
CP1ps	Space-like O(αs2) pure-singlet unpolarised splitting function
CP1qg	Space-like O(αs2) quark-gluon unpolarised splitting function
CP1Tgg	Time-like O(αs2) gluon-gluon unpolarised splitting function
CP1Tgq	Time-like O(αs2) gluon-quark unpolarised splitting function
CP1Tnsm	Time-like O(αs2) non-singlet-minus unpolarised splitting function
CP1Tnsp	Time-like O(αs2) non-singlet-plus unpolarised splitting function
CP1Tps	Time-like O(αs2) pure-singlet unpolarised splitting function
CP1Tqg	Time-like O(αs2) quark-gluon unpolarised splitting function
CP1transgg	Space-like O(αs2) gluon-gluon linearly polarised splitting function
CP1transnsm	Space-like O(αs2) non-singlet-minus transversely polarised splitting function
CP1transnsp	Space-like O(αs2) non-singlet-plus transversely polarised splitting function
CP1Ttransnsm	Time-like O(αs2) non-singlet-minus transversely polarised splitting function
CP1Ttransnsp	Time-like O(αs2) non-singlet-plus transversely polarised splitting function
CP2gg	Space-like O(αs3) gluon-gluon unpolarised splitting function
CP2gq	Space-like O(αs3) gluon-quark unpolarised splitting function
CP2nsm	Space-like O(αs3) non-singlet-minus unpolarised splitting function
CP2nsp	Space-like O(αs3) non-singlet-plus unpolarised splitting function
CP2nss	Space-like O(αs3) non-singlet-valence unpolarised splitting function minus non-singlet-minus unpolarised splitting function
CP2polgg	Space-like O(αs3) gluon-gluon longitudinally polarised splitting function
CP2polgq	Space-like O(αs3) gluon-quark longitudinally polarised splitting function
CP2polnsm	Space-like O(αs3) non-singlet-minus longitudinally polarised splitting function. This is equal to the non-singlet-plus unpolarised splitting function
CP2polnsp	Space-like O(αs3) non-singlet-plus longitudinally polarised splitting function. This is equal to the non-singlet-minus unpolarised splitting function
CP2polnss	Space-like O(αs3) non-singlet-valence longitudinally polarised splitting function minus non-singlet-minus longitudinally polarised splitting function
CP2polps	Space-like O(αs3) pure-singlet longitudinally polarised splitting function
CP2polqg	Space-like O(αs3) quark-gluon longitudinally polarised splitting function
CP2ps	Space-like O(αs3) pure-singlet unpolarised splitting function
CP2qg	Space-like O(αs3) quark-gluon unpolarised splitting function
CP2Tgg	Time-like O(αs3) gluon-gluon unpolarised splitting function
CP2Tgq	Time-like O(αs3) gluon-quark unpolarised splitting function
CP2Tnsm	Time-like O(αs3) non-singlet-minus unpolarised splitting function
CP2Tnsp	Time-like O(αs3) non-singlet-plus unpolarised splitting function
CP2Tnss	Time-like O(αs3) non-singlet-valence unpolarised splitting function minus non-singlet-minus unpolarised splitting function
CP2Tps	Time-like O(αs3) pure-singlet unpolarised splitting function
CP2Tqg	Time-like O(αs3) quark-gluon unpolarised splitting function
CP3gg	Space-like O(αs4) gluon-gluon unpolarised splitting function
CP3gq	Space-like O(αs4) gluon-quark unpolarised splitting function
CP3nsm	Space-like O(αs4) non-singlet-minus unpolarised splitting function
CP3nsp	Space-like O(αs4) non-singlet-plus unpolarised splitting function
CP3nss	Space-like O(αs4) non-singlet-valence unpolarised splitting function minus non-singlet-minus unpolarised splitting function
CP3ps	Space-like O(αs4) pure-singlet unpolarised splitting function
CP3qg	Space-like O(αs4) quark-gluon unpolarised splitting function
CPgpd0gg	O(αs) gluon-gluon unpolarised splitting function
CPgpd0gq	O(αs) gluon-quark unpolarised splitting function
CPgpd0ns	O(αs) non-singlet unpolarised evolution kernel
CPgpd0polgg	O(αs) gluon-gluon polarised splitting function
CPgpd0polgq	O(αs) gluon-quark polarised splitting function
CPgpd0polns	O(αs) non-singlet polarised evolution kernel
CPgpd0polqg	O(αs) quark-gluon polarised splitting function
CPgpd0polqq	O(αs) quark-quark polarised splitting function
CPgpd0qg	O(αs) quark-gluon unpolarised splitting function
CPgpd0qq	O(αs) quark-quark unpolarised splitting function
CPgpd0transgg	O(αs) gluon-gluon linearly polarised splitting function
CPgpd0transns	O(αs) non-singlet polarised evolution kernel
CPgpd0transqq	O(αs) quark-quark transversely polarised splitting function
CQGrid	The template class QGrids is a mother class for the interpolation in Q. This class also implements methods for the subgrid interpolation relevant for example in a VFNS evolution
CSet	The Set template class allocates a collection of objects of type T along the ConvolutionMap and provides the methods to perform operations between different types of objects T
CStructureFunctionObjects	Structure that contains all the precomputed quantities needed to compute the DIS structure functions, i.e. the perturbative coefficients of the coefficient functions for F2, FL, and xF3
CSubGrid	Class for the x-space interpolation SubGrids
CTabulateObject	The template TabulateObject class is a derived of the QGrid class that tabulates on object of type T (it can be a double, a Distribution, an Operator, Set<Distribution>, a Set<Operator>) over a grid in Q, taking into account the possible presence of thresholds, and provides the method to evaluate the tabulated object at any generic value of Q
Cterm	The term structure that contains all the objects of a single term of a double object
CTimer	Computes the time elapsed between start and stop
CTmdObjects	Structure that contains all precomputed quantities needed to perform the TMD evolution, matching to the collinear PDFs, and computation of cross sections, i.e. the perturbative coefficients of matching functions, all anomalous dimensions, and hard functions
CTwoBodyPhaseSpace	Class for the calculation of the phase-space reduction factor due to cuts on the single outgoing lepton in Drell-Yan production. The relevant process is: γ(q) → l+(k1) + l-(k2) with: kT,1(2) > pT,min,1(2) < ηmin η1(2) < ηmax