►Capfel::ConvolutionMap | Encapsulates the set of rules to multiply a sets of operators with a set of distributions |
Capfel::DISCCBasis | Derived of ConvolutionMap specialised for the computation of the CC DIS structure functions |
Capfel::DISNCBasis | Derived of ConvolutionMap specialised for the computation of the NC DIS structure functions |
Capfel::DiagonalBasis | Simplest derivation of ConvolutionMap meant to essentially perform a scalar product of two sets of objects |
Capfel::EvolBasisPlusMinus | Derives from ConvolutionMap and implements a basis in which plus (q+qbar) and minus (q-qbar) combinations are fully coupled |
Capfel::EvolutionBasisQCD | Derived of ConvolutionMap specialised for the DGLAP evolution of distributions using the QCD evolution basis |
Capfel::EvolutionOperatorBasisQCD | Derived of ConvolutionMap specialised for the DGLAP evolution of operators using the QCD evolution basis |
Capfel::EvolveDistributionsBasisQCD | Derived of ConvolutionMap specialised to match a set of evolution operators to a set a initial-scale distributions |
Capfel::MatchingBasisQCD | Derived of ConvolutionMap specialised for the matching of distributions using the QCD evolution basis and without assuming that intrinsic heavy quark contributions vanish |
Capfel::MatchingOperatorBasisQCD | Derived of ConvolutionMap specialised for the matching of the evolution of operators at the heavy-quark thresholds using the QCD evolution basis |
Capfel::Observable< T >::ConvolutionPair | This structure contains a pair of sets of coefficient functions and of objects |
Capfel::DglapObjects | 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 |
Capfel::DoubleExponentialQuadrature | DE-Quadrature Numerical automatic integrator for improper integral using double dxponential (DE) quadrature. The code is a manipulation of the code linked here: |
Capfel::DoubleObject< T, U > | 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 |
Capfel::EvolutionSetup | The EvolutionSetup structure is a collection of all possible evolution parameters |
►Capfel::Expression | Encapsulates in a proper form a given analytic expression in such a way that it can be transformed into an operator |
Capfel::ANS2qqH_0 | O(αs2) constant term of eq (B.4) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::ANS2qqH_L | O(αs2) term propotional to ln(μ2/m2) of eq (B.4) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::ANS2qqH_L2 | O(αs2) term propotional to ln2(μ2/m2) of eq (B.4) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::ANS3qqH_0 | O(αs3) constant term |
Capfel::APS2Hq_0 | O(αs2) constant term of eq (B.1) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::APS2Hq_L | O(αs2) term propotional to ln(μ2/m2) of eq (B.1) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::APS2Hq_L2 | O(αs2) term propotional to ln2(μ2/m2) of eq (B.1) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::APS3Hq_0 | O(αs3) constant term |
Capfel::AS1HH_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 |
Capfel::AS1HH_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 |
Capfel::AS1Hg_L | O(αs) term propotional to ln(μ2/m2) of eq. (B.2) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS1gH_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 |
Capfel::AS1gH_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 |
Capfel::AS1ggH_L | O(αs) term propotional to ln(μ2/m2) of eq (B.6) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS1polHH_0 | O(αs) constant term for the HH matching |
Capfel::AS1polHH_L | O(αs) term propotional to ln(μ2/m2) for the HH matching |
Capfel::AS1polHg_L | O(αs) term propotional to ln(μ2/m2) |
Capfel::AS1polgH_0 | O(αs) constant term for the gH matching |
Capfel::AS1polgH_L | O(αs) term propotional to ln(μ2/m2) for the gH matching |
Capfel::AS1polggH_L | O(αs) term propotional to ln(μ2/m2) |
Capfel::AS2Hg_0 | O(αs2) constant term of eq (B.3) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS2Hg_L | O(αs2) term propotional to ln(μ2/m2) of eq (B.3) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS2Hg_L2 | O(αs2) term propotional to ln2(μ2/m2) of eq (B.3) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS2ggH_0 | O(αs2) constant term of eq (B.7) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS2ggH_L | O(αs2) term propotional to ln(μ2/m2) of eq (B.7) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS2ggH_L2 | O(αs2) term propotional to ln2(μ2/m2) of eq (B.7) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS2gqH_0 | O(αs2) constant term of eq (B.5) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS2gqH_L | O(αs2) term propotional to ln(μ2/m2) of eq (B.5) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS2gqH_L2 | O(αs2) term propotional to ln2(μ2/m2) of eq (B.5) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::AS3Hg_0 | O(αs3) constant term |
Capfel::AS3ggH_0 | O(αs3) constant term |
Capfel::AS3gqH_0 | O(αs3) constant term |
Capfel::ATS1HH_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 |
Capfel::ATS1HH_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 |
Capfel::ATS1Hg_0 | O(αs) constant term of eq. (15) of https://arxiv.org/pdf/hep-ph/0504192.pdf |
Capfel::ATS1Hg_L | O(αs) term propotional to ln(μ2/m2) of eq. (15) of https://arxiv.org/pdf/hep-ph/0504192.pdf |
Capfel::ATS1gH_L | O(αs) term propotional to ln(μ2/m2) of eq. (B.2) of https://arxiv.org/pdf/hep-ph/9612398.pdf |
Capfel::ATS1ggH_L | O(αs) term propotional to ln(μ2/m2) of eq. (22) of https://arxiv.org/pdf/hep-ph/0504192.pdf |
Capfel::C1ggff | 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) |
Capfel::C1ggpdf | 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) |
Capfel::C1ggpdfBM | The O(αs) gluon-gluon matching function for linearly polarised gluon PDF (reference: https://arxiv.org/pdf/1907.03780.pdf) |
Capfel::C1ggpdfg1 | The O(αs) gluon-gluon matching function for g1 PDFs (reference: https://arxiv.org/pdf/1702.06558.pdf) |
Capfel::C1gqff | 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) |
Capfel::C1gqpdf | 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) |
Capfel::C1gqpdfBM | The O(αs) gluon-quark matching function for linearly polarised gluon PDF (reference: https://arxiv.org/pdf/1907.03780.pdf) |
Capfel::C1gqpdfg1 | The O(αs) gluon-quark matching function for g1 PDFs (reference: https://arxiv.org/pdf/1702.06558.pdf) |
Capfel::C1nsff | 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) |
Capfel::C1nspdf | 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) |
Capfel::C1nspdfSivers | The O(αs) non-singlet matching function for Sivers PDFs (see Eq. (A.9) of https://arxiv.org/pdf/2009.10710.pdf) |
Capfel::C1nspdfg1 | The O(αs) non-singlet matching function for g1 PDFs (reference: https://arxiv.org/pdf/1702.06558.pdf) |
Capfel::C1qgff | 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) |
Capfel::C1qgpdf | 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) |
Capfel::C1qgpdfg1 | The O(αs) quark-gluon matching function for g1 PDFs (reference: https://arxiv.org/pdf/1702.06558.pdf) |
Capfel::C21Tg | O(αs) gluon coefficient function for F2 in SIA |
Capfel::C21Tns | O(αs) non-singlet coefficient function for F2 in SIA |
Capfel::C21g | O(αs) gluon coefficient function for F2 |
Capfel::C21ns | O(αs) non-singlet coefficient function for F2 |
Capfel::C22Tg | O(αs2) gluon coefficient function for F2 in SIA |
Capfel::C22Tnsp | O(αs2) non-singlet-plus coefficient function for F2 in SIA |
Capfel::C22Tps | O(αs2) pure-singlet coefficient function for F2 in SIA |
Capfel::C22g | O(αs2) gluon coefficient function for F2 |
Capfel::C22nsm | O(αs2) non-singlet-minus coefficient function for F2 |
Capfel::C22nsp | O(αs2) non-singlet-plus coefficient function for F2 |
Capfel::C22ps | O(αs2) pure-singlet coefficient function for F2 |
Capfel::C23g | O(αs3) gluon coefficient function for F2 |
Capfel::C23nsm | O(αs3) non-singlet-minus coefficient function for F2 |
Capfel::C23nsp | O(αs3) non-singlet-plus coefficient function for F2 |
Capfel::C23ps | O(αs3) pure-singlet coefficient function for F2 |
Capfel::C2ggff | 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) |
Capfel::C2ggpdf | The O(αs2) gluon-gluon matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C2ggpdfBM | The O(αs2) gluon-gluon matching function for linearly polarised gluon PDFs (reference: https://arxiv.org/pdf/1907.03780.pdf) |
Capfel::C2gqff | 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) |
Capfel::C2gqpdf | The O(αs2) gluon-quark matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C2gqpdfBM | The O(αs2) gluon-quark matching function for linearly polarised gluon PDF (reference: https://arxiv.org/pdf/1907.03780.pdf) |
Capfel::C2nsmff | 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) |
Capfel::C2nsmpdf | The O(αs2) valence minus matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C2nspff | 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) |
Capfel::C2nsppdf | The O(αs2) valence plus matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C2psff | 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) |
Capfel::C2pspdf | The O(αs2) pure-singlet matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C2qgff | 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) |
Capfel::C2qgpdf | The O(αs2) quark-gluon matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C31Tns | O(αs) non-singlet coefficient function for F3 in SIA |
Capfel::C31ns | O(αs) non-singlet coefficient function for F3 |
Capfel::C32Tnsp | O(αs2) non-singlet-plus coefficient function for F3 in SIA |
Capfel::C32nsm | O(αs2) non-singlet-minus coefficient function for F3 |
Capfel::C32nsp | O(αs2) non-singlet-plus coefficient function for F3 |
Capfel::C33nsm | O(αs3) non-singlet-minus coefficient function for F3 |
Capfel::C33nsp | O(αs3) non-singlet-plus coefficient function for F3 |
Capfel::C33nsv | O(αs3) total-valence coefficient function for F3 |
Capfel::C3ggff | The O(αs3) gluon-gluon matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3ggpdf | The O(αs3) gluon-gluon matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3gqff | The O(αs3) gluon-quark matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3gqpdf | The O(αs3) gluon-quark matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3nsmff | The O(αs3) valence minus matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3nsmpdf | The O(αs3) valence minus matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3nspff | The O(αs3) valence plus matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3nsppdf | The O(αs3) valence plus matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3psff | The O(αs3) pure-singlet matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3pspdf | The O(αs3) pure-singlet matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3pvff | The O(αs3) pure-valence matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3pvpdf | The O(αs3) pure-valence matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3qgff | The O(αs3) quark-gluon matching function for FFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::C3qgpdf | The O(αs3) quark-gluon matching function for PDFs (reference: https://arxiv.org/pdf/2012.03256.pdf) |
Capfel::CL1Tg | O(αs) gluon coefficient function for FL in SIA |
Capfel::CL1Tns | O(αs) non-singlet coefficient function for FL in SIA |
Capfel::CL1g | O(αs) gluon coefficient function for FL |
Capfel::CL1ns | O(αs) non-singlet coefficient function for FL |
Capfel::CL2Tg | O(αs2) gluon coefficient function for FL in SIA |
Capfel::CL2Tnsp | O(αs2) non-singlet-plus coefficient function for FL in SIA |
Capfel::CL2Tps | O(αs2) pure-singlet coefficient function for FL in SIA |
Capfel::CL2g | O(αs2) gluon coefficient function for FL |
Capfel::CL2nsm | O(αs2) non-singlet-minus coefficient function for FL |
Capfel::CL2nsp | O(αs2) non-singlet-plus coefficient function for FL |
Capfel::CL2ps | O(αs2) pure-singlet coefficient function for FL |
Capfel::CL3g | O(αs3) gluon coefficient function for FL |
Capfel::CL3nsm | O(αs3) non-singlet-minus coefficient function for FL |
Capfel::CL3nsp | O(αs3) non-singlet-plus coefficient function for FL |
Capfel::CL3ps | O(αs3) pure-singlet coefficient function for FL |
Capfel::Cgtmd1gg | The O(αs) gluon-gluon unpolarised matching function for GTMDs |
Capfel::Cgtmd1gq | The O(αs) gluon-quark unpolarised matching function for GTMDs |
Capfel::Cgtmd1lingg | The O(αs) gluon-gluon linearly polarised matching function for GTMDs |
Capfel::Cgtmd1linpolgg | The O(αs) gluon(lin)-gluon(long pol) matching function for GTMDs |
Capfel::Cgtmd1linpolgq | The O(αs) gluon(lin)-quark(long pol) matching function for GTMDs |
Capfel::Cgtmd1linunpgg | The O(αs) gluon(lin)-gluon(unpol) matching function for GTMDs |
Capfel::Cgtmd1linunpgq | The O(αs) gluon(lin)-quark(unpol) matching function for GTMDs |
Capfel::Cgtmd1ns | The O(αs) non-singlet unpolarised matching function for GTMDs |
Capfel::Cgtmd1polgg | The O(αs) gluon-gluon longitudinally polarised matching function for GTMDs |
Capfel::Cgtmd1polgq | The O(αs) gluon-quark longitudinally polarised matching function for GTMDs |
Capfel::Cgtmd1polns | The O(αs) non-singlet longitudinally polarised matching function for GTMDs |
Capfel::Cgtmd1polqg | The O(αs) quark-gluon longitudinally polarised matching function for GTMDs |
Capfel::Cgtmd1polqq | The O(αs) quark-quark longitudinally polarised matching function for GTMDs |
Capfel::Cgtmd1qg | The O(αs) quark-gluon unpolarised matching function for GTMDs |
Capfel::Cgtmd1qq | The O(αs) quark-quark unpolarised matching function for GTMDs |
Capfel::Cm021gNC_c | O(αs) gluon coefficient function for F2. Constant term |
Capfel::Cm021gNC_l | O(αs) gluon coefficient function for F2. Single-log term |
Capfel::Cm022gNC_c | O(αs2) gluon coefficient function for F2. Constant term |
Capfel::Cm022gNC_f | O(αs2) gluon coefficient function for F2. Single-log(μF) term |
Capfel::Cm022gNC_l | O(αs2) gluon coefficient function for F2. Single-log term |
Capfel::Cm022gNC_l2 | O(αs2) gluon coefficient function for F2. Double-log term |
Capfel::Cm022gNC_lf | O(αs2) gluon coefficient function for F2. Mixed-double-log term |
Capfel::Cm022nsNC_c | O(αs2) non-singlet coefficient function for F2. Constant term |
Capfel::Cm022nsNC_l | O(αs2) non-singlet coefficient function for F2. Single-log term |
Capfel::Cm022nsNC_l2 | O(αs2) non-singlet coefficient function for F2. Double-log term |
Capfel::Cm022psNC_c | O(αs2) pure-singlet coefficient function for F2. Constant term |
Capfel::Cm022psNC_f | O(αs2) pure-singlet coefficient function for F2. Single-log(μF) term |
Capfel::Cm022psNC_l | O(αs2) pure-singlet coefficient function for F2. Single-log term |
Capfel::Cm022psNC_l2 | O(αs2) pure-singlet coefficient function for F2. Double-log term |
Capfel::Cm022psNC_lf | O(αs2) pure-singlet coefficient function for F2. Mixed-double-log term |
Capfel::Cm023gNC_c | O(αs3) constant term of gluon coefficient function for F2. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm023gNC_l | O(αs3) linear log of gluon coefficient function for F2. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm023gNC_l2 | O(αs3) quadratic log of gluon coefficient function for F2. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm023gNC_l3 | O(αs3) cubic log of gluon coefficient function for F2. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm023psNC_c | O(αs3) constant term of pure-single coefficient function for F2. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm023psNC_l | O(αs3) linear log of pure-single coefficient function for F2. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm023psNC_l2 | O(αs3) quadratic log of pure-single coefficient function for F2. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm023psNC_l3 | O(αs3) cubic log of pure-single coefficient function for F2. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm0L1gNC_c | O(αs) gluon coefficient function for FL. Constant term |
Capfel::Cm0L2gNC_c | O(αs2) gluon coefficient function for FL. Constant term |
Capfel::Cm0L2gNC_f | O(αs2) gluon coefficient function for FL. Single-log(μF) term |
Capfel::Cm0L2gNC_l | O(αs2) gluon coefficient function for FL. Single-log term |
Capfel::Cm0L2nsNC_c | O(αs2) non-singlet coefficient function for FL. Constant term |
Capfel::Cm0L2nsNC_l | O(αs2) non-singlet coefficient function for FL. Single-log term |
Capfel::Cm0L2psNC_c | O(αs2) pure-singlet coefficient function for FL. Constant term |
Capfel::Cm0L2psNC_f | O(αs2) pure-singlet coefficient function for FL. Single-log(μF) term |
Capfel::Cm0L2psNC_l | O(αs2) pure-singlet coefficient function for FL. Single-log term |
Capfel::Cm0L3gNC_c | O(αs3) constant term of gluon coefficient function for FL. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm0L3gNC_l | O(αs3) linear log term of gluon coefficient function for FL. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm0L3gNC_l2 | O(αs3) quadratic log term of gluon coefficient function for FL. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm0L3psNC_c | O(αs3) constant term of pure-single coefficient function for FL. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm0L3psNC_l | O(αs3) linear log of pure-single coefficient function for FL. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm0L3psNC_l2 | O(αs3) quadratic log of pure-single coefficient function for FL. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm0sx23gNC | O(αs3) gluon coefficient function for F2 at Q >> m and small x. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm0sx23psNC | O(αs3) pure-singlet coefficient function for F2 at Q >> m and small x. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm0sxL3gNC | O(αs3) gluon coefficient function for FL at Q >> m and small x. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm0sxL3psNC | O(αs3) pure-singlet coefficient function for FL at Q >> m and small x. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cm11ns | O(αs) non-singlet coefficient function for 2xF1. The relevant function is in Eq. (C4) of https://arxiv.org/pdf/hep-ph/9805233.pdf |
Capfel::Cm21gCC | O(αs) gluon coefficient function for F2 |
Capfel::Cm21gNC | 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' |
Capfel::Cm21ns | O(αs) non-singlet coefficient function for F2. The relevant function is in Eq. (C4) of https://arxiv.org/pdf/hep-ph/9805233.pdf |
Capfel::Cm21qCC | O(αs) quark coefficient function for F2 |
Capfel::Cm22bargNC | O(αs2) gluon coefficient function proportional to ln(Q2/M2) for F2. Uses the fortran routines in 'src/dis/hqcoef.f' |
Capfel::Cm22barpsNC | O(αs2) pure-singlet coefficient function proportional to ln(Q2/M2) for F2. Uses the fortran routines in 'src/dis/hqcoef.f' |
Capfel::Cm22gNC | O(αs2) gluon coefficient function for F2. Uses the fortran routines in 'src/dis/hqcoef.f' |
Capfel::Cm22nsNC | 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' |
Capfel::Cm22psNC | O(αs2) pure-singlet coefficient function for F2. Uses the fortran routines in 'src/dis/hqcoef.f' |
Capfel::Cm2a3gNC | Approximated O(αs3) gluon coefficient function for F2 |
Capfel::Cm2a3psNC | Approximated O(αs3) pure-singlet coefficient function for F2 |
Capfel::Cm31gCC | O(αs) gluon coefficient function for xF3 |
Capfel::Cm31ns | O(αs) non-singlet coefficient function for F3. The relevant function is in Eq. (C4) of https://arxiv.org/pdf/hep-ph/9805233.pdf |
Capfel::Cm31qCC | O(αs) quark coefficient function for xF3 |
Capfel::CmL1gCC | O(αs) gluon coefficient function for FL |
Capfel::CmL1gNC | O(αs) gluon coefficient function for FL |
Capfel::CmL1ns | 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 |
Capfel::CmL1qCC | O(αs) quark coefficient function for FL |
Capfel::CmL2bargNC | O(αs2) gluon coefficient function proportional to ln(Q2/M2) for FL. Uses the fortran routines in 'src/dis/hqcoef.f' |
Capfel::CmL2barpsNC | O(αs2) pure-singlet coefficient function proportional to ln(Q2/M2) for FL. Uses the fortran routines in 'src/dis/hqcoef.f' |
Capfel::CmL2gNC | O(αs2) gluon coefficient function for FL. Uses the fortran routines in 'src/dis/hqcoef.f' |
Capfel::CmL2nsNC | 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' |
Capfel::CmL2psNC | O(αs2) pure-singlet coefficient function for FL. Uses the fortran routines in 'src/dis/hqcoef.f' |
Capfel::CmLa3gNC | Approximated O(αs3) gluon coefficient function for FL |
Capfel::CmLa3psNC | Approximated O(αs3) pure-singlet coefficient function for FL |
Capfel::Cmsx23gNC | O(αs3) gluon coefficient function for F2 at small x. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cmsx23psNC | O(αs3) pure-singlet coefficient function for F2 at small x. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::CmsxL3gNC | O(αs3) gluon coefficient function for FL at small x. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::CmsxL3psNC | O(αs3) pure-singlet coefficient function for FL at small x. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::Cmth23gNC | O(αs3) gluon coefficient function for F2 near threshold. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::CmthL3gNC | O(αs3) gluon coefficient function for FL near threshold. Reference: https://arxiv.org/pdf/1205.5727 |
Capfel::G11g | O(αs) gluon coefficient function for for g1 |
Capfel::G11ns | O(αs) non-singlet coefficient function for g1 |
Capfel::G12g | O(αs2) gluon coefficient function for F2 |
Capfel::G12nsp | O(αs2) non-singlet-plus coefficient function for F2 |
Capfel::G12ps | O(αs2) pure-singlet coefficient function for F2 |
Capfel::G41ns | O(αs) non-singlet coefficient function for g4 |
Capfel::GL1ns | O(αs) non-singlet coefficient function for gL |
Capfel::Identity | Derived class from Expression to implement the Identity operator (delta function) |
Capfel::Null | Derived class from Expression to implement the Null operator (zero) |
Capfel::P0Tgg | Time-like O(αs) gluon-gluon unpolarised splitting function |
Capfel::P0Tgq | Time-like O(αs) gluon-quark unpolarised splitting function |
Capfel::P0Tns | Time-like O(αs) non-singlet unpolarised splitting function |
Capfel::P0Tqg | Time-like O(αs) quark-gluon unpolarised splitting function |
Capfel::P0Ttransns | Time-like O(αs) non-singlet transversely polarised splitting function |
Capfel::P0gg | Space-like O(αs) gluon-gluon unpolarised splitting function |
Capfel::P0gq | Space-like O(αs) gluon-quark unpolarised splitting function |
►Capfel::P0ns | Space-like O(αs) non-singlet unpolarised splitting function |
Capfel::P0polns | Space-like O(αs) non-singlet longitudinally polarised splitting function. This is equal to the non-singlet unpolarised splitting function |
Capfel::P0polgg | Space-like O(αs) gluon-gluon longitudinally polarised splitting function |
Capfel::P0polgq | Space-like O(αs) gluon-quark longitudinally polarised splitting function |
Capfel::P0polqg | Space-like O(αs) quark-gluon longitudinally polarised splitting function |
Capfel::P0qg | Space-like O(αs) quark-gluon unpolarised splitting function |
Capfel::P0transgg | Space-like O(αs) gluon-gluon linearly polarised splitting function |
Capfel::P0transns | Space-like O(αs) non-singlet transversely polarised splitting function |
Capfel::P1Tgg | Time-like O(αs2) gluon-gluon unpolarised splitting function |
Capfel::P1Tgq | Time-like O(αs2) gluon-quark unpolarised splitting function |
►Capfel::P1Tnsp | Time-like O(αs2) non-singlet-plus unpolarised splitting function |
Capfel::P1Tnsm | Time-like O(αs2) non-singlet-minus unpolarised splitting function |
Capfel::P1Tps | Time-like O(αs2) pure-singlet unpolarised splitting function |
Capfel::P1Tqg | Time-like O(αs2) quark-gluon unpolarised splitting function |
►Capfel::P1Ttransnsp | Time-like O(αs2) non-singlet-plus transversely polarised splitting function |
Capfel::P1Ttransnsm | Time-like O(αs2) non-singlet-minus transversely polarised splitting function |
Capfel::P1gg | Space-like O(αs2) gluon-gluon unpolarised splitting function |
Capfel::P1gq | Space-like O(αs2) gluon-quark unpolarised splitting function |
►Capfel::P1nsp | Space-like O(αs2) non-singlet-plus unpolarised splitting function |
►Capfel::P1nsm | Space-like O(αs2) non-singlet-minus unpolarised splitting function |
Capfel::P1polnsp | Space-like O(αs2) non-singlet-plus longitudinally polarised splitting function. This is equal to the non-singlet-minus unpolarised splitting function |
Capfel::P1polnsm | Space-like O(αs2) non-singlet-minus longitudinally polarised splitting function. This is equal to the non-singlet-plus unpolarised splitting function |
Capfel::P1polgg | Space-like O(αs2) gluon-gluon longitudinally polarised splitting function |
Capfel::P1polgq | Space-like O(αs2) gluon-quark longitudinally polarised splitting function |
Capfel::P1polps | Space-like O(αs2) pure-singlet longitudinally polarised splitting function |
Capfel::P1polqg | Space-like O(αs2) quark-gluon longitudinally polarised splitting function |
Capfel::P1ps | Space-like O(αs2) pure-singlet unpolarised splitting function |
Capfel::P1qg | Space-like O(αs2) quark-gluon unpolarised splitting function |
Capfel::P1transgg | Space-like O(αs2) gluon-gluon linearly polarised splitting function |
►Capfel::P1transnsp | Space-like O(αs2) non-singlet-plus transversely polarised splitting function |
Capfel::P1transnsm | Space-like O(αs2) non-singlet-minus transversely polarised splitting function |
Capfel::P2Tgg | Time-like O(αs3) gluon-gluon unpolarised splitting function |
Capfel::P2Tgq | Time-like O(αs3) gluon-quark unpolarised splitting function |
Capfel::P2Tnsm | Time-like O(αs3) non-singlet-minus unpolarised splitting function |
Capfel::P2Tnsp | Time-like O(αs3) non-singlet-plus unpolarised splitting function |
Capfel::P2Tnss | Time-like O(αs3) non-singlet-valence unpolarised splitting function minus non-singlet-minus unpolarised splitting function |
Capfel::P2Tps | Time-like O(αs3) pure-singlet unpolarised splitting function |
Capfel::P2Tqg | Time-like O(αs3) quark-gluon unpolarised splitting function |
Capfel::P2gg | Space-like O(αs3) gluon-gluon unpolarised splitting function |
Capfel::P2gq | Space-like O(αs3) gluon-quark unpolarised splitting function |
►Capfel::P2nsm | Space-like O(αs3) non-singlet-minus unpolarised splitting function |
Capfel::P2polnsp | Space-like O(αs3) non-singlet-plus longitudinally polarised splitting function. This is equal to the non-singlet-minus unpolarised splitting function |
►Capfel::P2nsp | Space-like O(αs3) non-singlet-plus unpolarised splitting function |
Capfel::P2polnsm | Space-like O(αs3) non-singlet-minus longitudinally polarised splitting function. This is equal to the non-singlet-plus unpolarised splitting function |
Capfel::P2nss | Space-like O(αs3) non-singlet-valence unpolarised splitting function minus non-singlet-minus unpolarised splitting function |
Capfel::P2polgg | Space-like O(αs3) gluon-gluon longitudinally polarised splitting function |
Capfel::P2polgq | Space-like O(αs3) gluon-quark longitudinally polarised splitting function |
Capfel::P2polnss | Space-like O(αs3) non-singlet-valence longitudinally polarised splitting function minus non-singlet-minus longitudinally polarised splitting function |
Capfel::P2polps | Space-like O(αs3) pure-singlet longitudinally polarised splitting function |
Capfel::P2polqg | Space-like O(αs3) quark-gluon longitudinally polarised splitting function |
Capfel::P2ps | Space-like O(αs3) pure-singlet unpolarised splitting function |
Capfel::P2qg | Space-like O(αs3) quark-gluon unpolarised splitting function |
Capfel::P3gg | Space-like O(αs4) gluon-gluon unpolarised splitting function. Parameterisation determined in https://arxiv.org/pdf/2310.05744.pdf |
Capfel::P3gq | Space-like O(αs4) gluon-quark unpolarised splitting function. Parameterisation determined in https://arxiv.org/pdf/2310.05744.pdf |
Capfel::P3nsm | Space-like O(αs4) non-singlet-minus unpolarised splitting function. Parameterisation determined in https://arxiv.org/pdf/1707.08315.pdf |
Capfel::P3nsp | Space-like O(αs4) non-singlet-plus unpolarised splitting function. Parameterisation determined in https://arxiv.org/pdf/1707.08315.pdf |
Capfel::P3nss | Space-like O(αs4) non-singlet-valence unpolarised splitting function. Parameterisation determined in https://arxiv.org/pdf/1707.08315.pdf |
Capfel::P3ps | Space-like O(αs4) pure-singlet unpolarised splitting function. Parameterisation determined in https://arxiv.org/pdf/2302.07593.pdf |
Capfel::P3qg | Space-like O(αs4) quark-gluon unpolarised splitting function. Parameterisation determined in https://arxiv.org/pdf/2307.04158.pdf |
Capfel::Pgpd0gg | O(αs) gluon-gluon unpolarised splitting function |
Capfel::Pgpd0gq | O(αs) gluon-quark unpolarised splitting function |
Capfel::Pgpd0ns | O(αs) non-singlet unpolarised evolution kernel |
Capfel::Pgpd0polgg | O(αs) gluon-gluon polarised splitting function |
Capfel::Pgpd0polgq | O(αs) gluon-quark polarised splitting function |
Capfel::Pgpd0polns | O(αs) non-singlet polarised evolution kernel |
Capfel::Pgpd0polqg | O(αs) quark-gluon polarised splitting function |
Capfel::Pgpd0polqq | O(αs) quark-quark polarised splitting function |
Capfel::Pgpd0qg | O(αs) quark-gluon unpolarised splitting function |
Capfel::Pgpd0qq | O(αs) quark-quark unpolarised splitting function |
Capfel::Pgpd0transgg | O(αs) gluon-gluon linearly polarised splitting function |
Capfel::Pgpd0transns | O(αs) non-singlet polarised evolution kernel |
Capfel::Pgpd0transqq | O(αs) quark-quark transversely polarised splitting function |
Capfel::ExtendedVector< T > | Class that extends vectors to negative indices |
Capfel::Grid | 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 |
Capfel::EvolutionSetup::GridParameters | Structure for the subgrid parameters |
Capfel::GtmdObjects | |
Capfel::InitialiseEvolution | 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 |
Capfel::Integrator | Performs unidimensional numerical integrations using the Guassian quadrature |
Capfel::Integrator2D | Performs two-dimensional numerical integrations using the Guassian quadrature |
►Capfel::Interpolator | 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 |
►Capfel::LagrangeInterpolator | Specialization of the Interpolator class using the lagrange interpolation procedure |
Capfel::Distribution | Defines one of the basic objects of APFEL++. This is essentially the discretisation of a function that can be conveniently used for convolutions |
Capfel::LHKnotArray | 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 |
Capfel::MatchedEvolution< T > | 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 |
►Capfel::MatchedEvolution< double > | |
Capfel::AlphaQCD | The AlphaQCD is a specialization class of the MatchedEvolution class for the computation of the QCD coupling running |
Capfel::AlphaQCDg | The AlphaQCDg is a specialization class of the MatchedEvolution class for the computation of the QCD coupling running using the analytic g functions |
Capfel::AlphaQCDxi | 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 |
Capfel::AlphaQED | The AlphaQED is a specialization class of the MatchedEvolution class for the computation of the QED coupling running |
►Capfel::MatchedEvolution< matrix< double > > | |
Capfel::AlphaQCDQED | The AlphaQCDQED is a specialization class of the MatchedEvolution class for the computation of the mixed evolution of QCD and QED |
►Capfel::MatchedEvolution< Set< T > > | |
Capfel::Dglap< T > | The Dglap class is specialization class of the MatchedEvolution class for the computation of the DGLAP evolution |
Capfel::matrix< T > | The matrix class is a simple implementation of 2d arrays based on a continous memory allocation. Elements are accessible throught the (i,j) operator |
Capfel::matrix< double > | |
Capfel::Observable< T > | 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 |
Capfel::OgataQuadrature | 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 |
Capfel::Operator | 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 |
►Capfel::QGrid< T > | 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 |
Capfel::TabulateObject< T > | 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 |
►Capfel::QGrid< apfel::Set< apfel::Distribution > > | |
Capfel::TabulateObject< apfel::Set< apfel::Distribution > > | |
Capfel::ConvolutionMap::rule | This structure contains the attribute of a single rule |
Capfel::Set< T > | 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 |
Capfel::Set< apfel::Distribution > | |
Capfel::Set< apfel::Operator > | |
Capfel::StructureFunctionObjects | 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 |
Capfel::SubGrid | Class for the x-space interpolation SubGrids |
Capfel::term< V, U > | The term structure that contains all the objects of a single term of a double object |
Capfel::Timer | Computes the time elapsed between start and stop |
Capfel::TmdObjects | 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 |
Capfel::TwoBodyPhaseSpace | 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
|