A class for \(O(\alpha^2\alpha_s)\) three-loop corrections to the EW precision observables. More...
#include <EWSMThreeLoopEW2QCD.h>
A class for \(O(\alpha^2\alpha_s)\) three-loop corrections to the EW precision observables.
This class handles three-loop mixed EW-QCD contributions of \(O(\alpha^2\alpha_s)\) to the following quantities, which are relevant to the EW precision observables:
where only \(\Delta\rho\) is non-zero in the current class. See also the description of EWSM class for their definitions.
Definition at line 34 of file EWSMThreeLoopEW2QCD.h.
Public Member Functions | |
| double | DeltaAlpha_l (const double s) const |
| Leptonic contribution of \(O(\alpha^2\alpha_s)\) to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}^{\alpha^2\alpha_s}(s)\). More... | |
| double | DeltaAlpha_t (const double s) const |
| Top-quark contribution of \(O(\alpha^2\alpha_s)\) to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}^{\alpha^2\alpha_s}(s)\). More... | |
| gslpp::complex | deltaKappa_rem_f (const Particle f, const double Mw_i) const |
| Remainder contribution of \(O(\alpha^2\alpha_s)\) to the effective couplings \(\kappa_Z^f\), denoted as \(\delta\kappa_{\mathrm{rem}}^{f,\, \alpha^2\alpha_s}\). More... | |
| double | DeltaR_rem (const double Mw_i) const |
| Remainder contribution of \(O(\alpha^2\alpha_s)\) to \(\Delta r\), denoted as \(\Delta r_{\mathrm{rem}}^{\alpha^2\alpha_s}\). More... | |
| double | DeltaRho (const double Mw_i) const |
| Leading three-loop contribution of \(O(\alpha^2\alpha_s)\) to \(\Delta\rho\), denoted as \(\Delta\rho^{\alpha^2\alpha_s}\). More... | |
| gslpp::complex | deltaRho_rem_f (const Particle f, const double Mw_i) const |
| Remainder contribution of \(O(\alpha^2\alpha_s)\) to the effective couplings \(\rho_Z^f\), denoted as \(\delta\rho_{\mathrm{rem}}^{f,\, \alpha^2\alpha_s}\). More... | |
| EWSMThreeLoopEW2QCD (const EWSMcache &cache_i) | |
| Constructor. More... | |
Private Attributes | |
| const EWSMcache & | cache |
| A reference to an object of type EWSMcache. More... | |
| EWSMThreeLoopEW2QCD::EWSMThreeLoopEW2QCD | ( | const EWSMcache & | cache_i | ) |
Constructor.
| [in] | cache_i | a reference to an object of type EWSMcache |
Definition at line 11 of file EWSMThreeLoopEW2QCD.cpp.
| double EWSMThreeLoopEW2QCD::DeltaAlpha_l | ( | const double | s | ) | const |
Leptonic contribution of \(O(\alpha^2\alpha_s)\) to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}^{\alpha^2\alpha_s}(s)\).
This contribution vanishes at \(O(\alpha^2\alpha_s)\).
| [in] | s | invariant mass squared |
Definition at line 19 of file EWSMThreeLoopEW2QCD.cpp.
| double EWSMThreeLoopEW2QCD::DeltaAlpha_t | ( | const double | s | ) | const |
Top-quark contribution of \(O(\alpha^2\alpha_s)\) to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}^{\alpha^2\alpha_s}(s)\).
This contribution is not implemented, since it is tiny and negligible.
| [in] | s | invariant mass squared |
Definition at line 24 of file EWSMThreeLoopEW2QCD.cpp.
| gslpp::complex EWSMThreeLoopEW2QCD::deltaKappa_rem_f | ( | const Particle | f, |
| const double | Mw_i | ||
| ) | const |
Remainder contribution of \(O(\alpha^2\alpha_s)\) to the effective couplings \(\kappa_Z^f\), denoted as \(\delta\kappa_{\mathrm{rem}}^{f,\, \alpha^2\alpha_s}\).
This contribution is not implemented, since it is tiny and negligible.
| [in] | f | a lepton or quark |
| [in] | Mw_i | the \(W\)-boson mass |
Definition at line 74 of file EWSMThreeLoopEW2QCD.cpp.
| double EWSMThreeLoopEW2QCD::DeltaR_rem | ( | const double | Mw_i | ) | const |
Remainder contribution of \(O(\alpha^2\alpha_s)\) to \(\Delta r\), denoted as \(\Delta r_{\mathrm{rem}}^{\alpha^2\alpha_s}\).
This contribution is not implemented, since it is tiny and negligible.
| [in] | Mw_i | the \(W\)-boson mass |
Definition at line 63 of file EWSMThreeLoopEW2QCD.cpp.
| double EWSMThreeLoopEW2QCD::DeltaRho | ( | const double | Mw_i | ) | const |
Leading three-loop contribution of \(O(\alpha^2\alpha_s)\) to \(\Delta\rho\), denoted as \(\Delta\rho^{\alpha^2\alpha_s}\).
This function represents the leading three-loop mixed EW-QCD contribution of \(O(\alpha^2\alpha_s m_t^4/M_Z^4)\) to \(\Delta\rho\). Expressions are available for \(m_h=0\) in [171] and for \(m_h\approx m_t\) and \(m_h\gg m_t\) in [118].
| [in] | Mw_i | the \(W\)-boson mass |
Definition at line 29 of file EWSMThreeLoopEW2QCD.cpp.
| gslpp::complex EWSMThreeLoopEW2QCD::deltaRho_rem_f | ( | const Particle | f, |
| const double | Mw_i | ||
| ) | const |
Remainder contribution of \(O(\alpha^2\alpha_s)\) to the effective couplings \(\rho_Z^f\), denoted as \(\delta\rho_{\mathrm{rem}}^{f,\, \alpha^2\alpha_s}\).
This contribution is not implemented, since it is tiny and negligible.
| [in] | f | a lepton or quark |
| [in] | Mw_i | the \(W\)-boson mass |
Definition at line 68 of file EWSMThreeLoopEW2QCD.cpp.
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private |
A reference to an object of type EWSMcache.
Definition at line 113 of file EWSMThreeLoopEW2QCD.h.