yadism.coefficient_functions.light package
The coefficient functions definition is given in 4.2, [VVM05] (that is the main reference for their expression, i.e. all the formulas in this module) (the same of 1 in [MVV05]). The main reference for their expression is [MVV05].
Scale varitions main reference is [vNV00] and [vNV01].
Scale variations main reference is [MV00].
Note
Check the theory reference for details on Scale Variations
The source files (available in fortran) follow the notations in [MVV09] where the odd-N moments are called minus even if they correspond to \(\nu + \bar{\nu}\). This convention is changed in [DVMV16] where the complete N3LO CC results are presented for the first time. Referred equations are not always in agreement with the code conventions.
The code follows the notation:
- F3:
odd N: \(\nu + \bar{\nu}\), \(c_{ns,-}\) common for CC and NC (up to N3LO).
even N: \(\nu - \bar{\nu}\), \(c_{ns,+} = \delta + c_{ns,-}\) only for CC.
In \(c_{ns,+}\) the term fl02 has to be turned off for CC.
- F2, FL:
odd N: \(\nu - \bar{\nu}\), \(c_{ns,-} = - \delta + c_{ns,+}\) only for CC.
even N: \(\nu + \bar{\nu}\), \(c_{ns,+}\) common for CC and NC (up to N3LO).
The term fl11 has to be turned off for CC.
Subpackages
- yadism.coefficient_functions.light.n3lo package
- Submodules
- yadism.coefficient_functions.light.n3lo.common module
- yadism.coefficient_functions.light.n3lo.xc2ns3p module
- yadism.coefficient_functions.light.n3lo.xc2sg3p module
- yadism.coefficient_functions.light.n3lo.xc3ns3p module
- yadism.coefficient_functions.light.n3lo.xcdiff3p module
- yadism.coefficient_functions.light.n3lo.xclns3p module
- yadism.coefficient_functions.light.n3lo.xclsg3p module
- yadism.coefficient_functions.light.nlo package
- yadism.coefficient_functions.light.nnlo package
- Submodules
- yadism.coefficient_functions.light.nnlo.g1 module
- yadism.coefficient_functions.light.nnlo.xc2ns2p module
- yadism.coefficient_functions.light.nnlo.xc2sg2p module
- yadism.coefficient_functions.light.nnlo.xc3ns2p module
- yadism.coefficient_functions.light.nnlo.xclns2p module
- yadism.coefficient_functions.light.nnlo.xclsg2p module
- yadism.coefficient_functions.light.nnlo.xk3cnvp module
Submodules
yadism.coefficient_functions.light.f2_cc module
- class yadism.coefficient_functions.light.f2_cc.Gluon(ESF, nf)[source]
Bases:
Gluon- __annotations__ = {}
- class yadism.coefficient_functions.light.f2_cc.NonSingletEven(ESF, nf)[source]
Bases:
NonSinglet- __annotations__ = {}
- class yadism.coefficient_functions.light.f2_cc.NonSingletOdd(ESF, nf)[source]
Bases:
NonSinglet- __annotations__ = {}
yadism.coefficient_functions.light.f2_nc module
- class yadism.coefficient_functions.light.f2_nc.Gluon(ESF, nf)[source]
Bases:
LightBase- NLO()[source]
Reference: implements 4.4, [VVM05].
Note
2 * n_f is coming from momentum sum rule q_i -> {q_i, g} but g -> {g, q_i, bar{q_i} forall i}, so the 2 * n_f is needed to compensate for all the number of flavours plus antiflavours in which the gluon can go.
- __annotations__ = {}
- class yadism.coefficient_functions.light.f2_nc.GluonFL11(ESF, nf)[source]
Bases:
LightBaseGluon flavor class \(fl_{11}\).
- __annotations__ = {}
- class yadism.coefficient_functions.light.f2_nc.NonSinglet(ESF, nf)[source]
Bases:
LightBase- __annotations__ = {}
yadism.coefficient_functions.light.f3_cc module
Note that the source files (given in fortran) follow the notations in [MVV09] where the odd-N moments are called minus even if they correspond to :math:` u + ar{ u}`, while even-N moments are called plus even if they correspond to :math:` u - ar{ u}`. This convention is changed in [DVMV16] where the N3LO CC results are presented for the first time.
- class yadism.coefficient_functions.light.f3_cc.Gluon(*args, **_kwargs)[source]
Bases:
EmptyPartonicChannel- __annotations__ = {}
- class yadism.coefficient_functions.light.f3_cc.NonSingletEven(ESF, nf)[source]
Bases:
NonSinglet- __annotations__ = {}
- class yadism.coefficient_functions.light.f3_cc.NonSingletOdd(ESF, nf)[source]
Bases:
NonSinglet- __annotations__ = {}
- class yadism.coefficient_functions.light.f3_cc.Singlet(*args, **_kwargs)[source]
Bases:
EmptyPartonicChannel- __annotations__ = {}
yadism.coefficient_functions.light.f3_nc module
See f3_cc docstring for the name conventions.
- class yadism.coefficient_functions.light.f3_nc.Gluon(*args, **_kwargs)[source]
Bases:
EmptyPartonicChannel- __annotations__ = {}
- class yadism.coefficient_functions.light.f3_nc.NonSinglet(ESF, nf)[source]
Bases:
NonSinglet- __annotations__ = {}
- class yadism.coefficient_functions.light.f3_nc.Singlet(*args, **_kwargs)[source]
Bases:
EmptyPartonicChannel- __annotations__ = {}
yadism.coefficient_functions.light.fl_cc module
- class yadism.coefficient_functions.light.fl_cc.Gluon(ESF, nf)[source]
Bases:
Gluon- __annotations__ = {}
- class yadism.coefficient_functions.light.fl_cc.NonSingletEven(ESF, nf)[source]
Bases:
NonSinglet- __annotations__ = {}
- class yadism.coefficient_functions.light.fl_cc.NonSingletOdd(ESF, nf)[source]
Bases:
NonSinglet- __annotations__ = {}
yadism.coefficient_functions.light.fl_nc module
- class yadism.coefficient_functions.light.fl_nc.Gluon(ESF, nf)[source]
Bases:
LightBase- __annotations__ = {}
- class yadism.coefficient_functions.light.fl_nc.GluonFL11(ESF, nf)[source]
Bases:
LightBaseGluon flavor class \(fl_{11}\).
- __annotations__ = {}
- class yadism.coefficient_functions.light.fl_nc.NonSinglet(ESF, nf)[source]
Bases:
LightBase- __annotations__ = {}
yadism.coefficient_functions.light.g1_nc module
- class yadism.coefficient_functions.light.g1_nc.Gluon(ESF, nf)[source]
Bases:
LightBase- NLO()[source]
Reference: implements NLO-part of A.5, [ZvN94]. For a simpler expression, refer also to 9 of [dFS95].
Note
2 * n_f is coming from momentum sum rule q_i -> {q_i, g} but g -> {g, q_i, bar{q_i} forall i}, so the 2 * n_f is needed to compensate for all the number of flavours plus antiflavours in which the gluon can go.
- __annotations__ = {}
- class yadism.coefficient_functions.light.g1_nc.NonSinglet(ESF, nf)[source]
Bases:
LightBase- static NLO()[source]
Reference: implements the equivalence relation between \(g_1\) and \(F_3\) as explained in A.19 (and paragraph below) of [BdFP22]. For the explicit expressions, refer to A.1 of [ZvN94] and 15 of [dFS95].
- NNLO()[source]
Reference: implements the equivalence relation between \(g_1\) and \(F_3\) as explained in A.19 (and paragraph below) of [BdFP22]. For the explicit expressions, refer to A.1 of [ZvN94] and 15 of [dFS95].
- __annotations__ = {}
yadism.coefficient_functions.light.g4_nc module
- class yadism.coefficient_functions.light.g4_nc.Gluon(*args, **_kwargs)[source]
Bases:
EmptyPartonicChannel- __annotations__ = {}
- class yadism.coefficient_functions.light.g4_nc.NonSinglet(ESF, nf)[source]
Bases:
LightBase- __annotations__ = {}
- class yadism.coefficient_functions.light.g4_nc.Singlet(*args, **_kwargs)[source]
Bases:
EmptyPartonicChannel- __annotations__ = {}
- class yadism.coefficient_functions.light.g4_nc.Valence(*args, **_kwargs)[source]
Bases:
EmptyPartonicChannel- __annotations__ = {}
yadism.coefficient_functions.light.gl_nc module
- class yadism.coefficient_functions.light.gl_nc.Gluon(*args, **_kwargs)[source]
Bases:
EmptyPartonicChannel- __annotations__ = {}
- class yadism.coefficient_functions.light.gl_nc.NonSinglet(ESF, nf)[source]
Bases:
LightBase- __annotations__ = {}
- class yadism.coefficient_functions.light.gl_nc.Singlet(*args, **_kwargs)[source]
Bases:
EmptyPartonicChannel- __annotations__ = {}
- class yadism.coefficient_functions.light.gl_nc.Valence(*args, **_kwargs)[source]
Bases:
EmptyPartonicChannel- __annotations__ = {}
yadism.coefficient_functions.light.kernels module
- yadism.coefficient_functions.light.kernels.generate(esf, nf)[source]
Collect the light coefficient functions
- Parameters:
esf (EvaluatedStructureFunction) – kinematic point
nf (int) – number of light flavors
- Returns:
elems – list of elements
- Return type:
list(yadism.kernels.Kernel)
- yadism.coefficient_functions.light.kernels.nc_fl11_weights(coupling_constants, Q2, nf, skip_heavylight=False)[source]
Compute the NC weights for the flavor class \(fl_{11}\).
For the time being we don’t have such diagrams for parity violating structure functions.
- Parameters:
coupling_constants (CouplingConstants) – manager for coupling constants
Q2 (float) – W virtuality
nf (int) – number of light flavors
skip_heavylight (bool) – prevent the last quark to couple to the boson
- Returns:
weights – mapping pid -> weight for ns, g and s channel
- Return type:
- yadism.coefficient_functions.light.kernels.nc_weights(coupling_constants, Q2, nf, is_pv, skip_heavylight=False)[source]
Compute light NC weights.
- Parameters:
coupling_constants (CouplingConstants) – manager for coupling constants
Q2 (float) – W virtuality
nf (int) – number of light flavors
is_pv (bool) – True if observable violates parity conservation
skip_heavylight (bool) – prevent the last quark to couple to the boson
- Returns:
weights – mapping pid -> weight for ns, g and s channel
- Return type:
yadism.coefficient_functions.light.partonic_channel module
- class yadism.coefficient_functions.light.partonic_channel.LightBase(ESF, nf)[source]
Bases:
PartonicChannelLight partonic channel base class.
- __annotations__ = {}