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QQbar_threshold
contribution_factors Struct Reference

Multiplicative coefficients for the potentials and current matching coefficients. More...

Public Attributes

std::array< double, 3 > v_Coulomb = {{1.,1.,1.}}
 Corrections \(\hat{\cal V}_C^{(1)},\hat{\cal V}_C^{(2)},\hat{\cal V}_C^{(3)}\) to the colour Coulomb potential.
 
std::array< double, 2 > v_delta = {{1.,1.}}
 Corrections \(\hat{\cal V}_{1/m^2}^{(1)},\hat{\cal V}_{1/m^2}^{(2)}\) to the \(\delta\) (or \(1/m^2\)) potential.
 
std::array< double, 2 > v_r2inv = {{1.,1.}}
 Corrections \(\hat{\cal V}_{1/m}^{(1)},\hat{\cal V}_{1/m}^{(2)}\) to the \(1/r^2\) (or \(1/m\)) potential.
 
std::array< double, 2 > v_p2 = {{1.,1.}}
 Corrections \(\hat{\cal V}_{p}^{(1)},\hat{\cal V}_{p}^{(2)}\) to the momentum dependent potential.
 
std::array< double, 1 > v_kinetic = {{1.}}
 Kinetic corrections.
 
std::array< double, 1 > ultrasoft = {{1.}}
 Ultrasoft corrections.
 
std::array< double, 1 > v_Higgs = {{1.}}
 Higgs potential.
 
std::array< double, 1 > v_QED_Coulomb = {{1.}}
 Corrections due to the classical (QED) Coulomb potential.
 
std::array< double, 3 > cv = {{1.,1.,1.}}
 Corrections to the hard matching coefficient \(c_v\).
 
std::array< double, 2 > cv_Higgs = {{1.,1.}}
 Higgs corrections to the hard matching coefficient \(c_v\).
 
std::array< double, 1 > Cv_QED = {{1.}}
 QED corrections to hard matching with vector coupling to leptons.
 
std::array< double, 1 > Cv_WZ = {{1.}}
 W,Z corrections to hard matching with vector coupling to leptons.
 
std::array< double, 1 > Ca_QED = {{1.}}
 QED corrections to hard matching with axialvector coupling to leptons.
 
std::array< double, 1 > Ca_WZ = {{1.}}
 W,Z corrections to hard matching with axialvector coupling to leptons.
 
std::array< double, 2 > dv = {{1.,1.}}
 Sub-leading hard matching coefficient \(d_v\).
 
std::array< double, 1 > ca = {{1.}}
 P-wave hard matching coefficient \(c_a\).
 

Detailed Description

Multiplicative coefficients for the potentials and current matching coefficients.

E.g. setting

options opt;
opt.contributions.v_delta = {{0.0, 1.0}};

implies that corrections due to the leading-order delta potential are multiplied by zero, i.e. effectively discarded, but corrections from the next-to-leading delta potential are kept.

The contributions are defined as in [8].