master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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A class for testing SM radiative corrections to the EW precision obsrvables. More...
#include <EWSM_Output.h>
Inheritance diagram for EWSM_Output:A class for testing SM radiative corrections to the EW precision obsrvables.
Definition at line 22 of file EWSM_Output.h.
Public Member Functions | |
| EWSM_Output (const StandardModel &SM_in) | |
| Constructor. More... | |
| void | outputEachDeltaKappaZ (const double f_AlphaToGF, const double cW2overSW2, const double DeltaRho[StandardModel::orders_EW_size], const double deltaKappa_rem[StandardModel::orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb, const double taub[StandardModel::orders_EW_size], const double ZbbSubtract, const double Zgamma_EW2) const |
| void | outputEachDeltaKappaZ_l (const QCD::lepton l, const double Mw_i) const |
| void | outputEachDeltaKappaZ_q (const QCD::quark q, const double Mw_i) const |
| void | outputEachDeltaR (const double Mw_i) const |
| void | outputEachDeltaRhoZ (const double f_AlphaToGF, const double DeltaRho[StandardModel::orders_EW_size], const double deltaRho_rem[StandardModel::orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb, const double taub[StandardModel::orders_EW_size], const double ZbbSubtract) const |
| void | outputEachDeltaRhoZ_l (const QCD::lepton l, const double Mw_i) const |
| void | outputEachDeltaRhoZ_q (const QCD::quark q, const double Mw_i) const |
| Public Member Functions inherited from StandardModel | |
| virtual const double | A_f (const Particle f) const |
| The left-right asymmetry in \(e^+e^-\to Z\to \ell \bar{\ell}\) at the \(Z\)-pole, \(\mathcal{A}_\ell\). More... | |
| virtual const double | AFB (const Particle f) const |
| gslpp::complex | AH_f (const double tau) const |
| Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | AH_W (const double tau) const |
| W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More... | |
| gslpp::complex | AHZga_f (const double tau, const double lambda) const |
| Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | AHZga_W (const double tau, const double lambda) const |
| W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| const double | Ale (double mu, orders order, bool Nf_thr=true) const |
| The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More... | |
| const double | ale_OS (const double mu, orders order=FULLNLO) const |
| The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More... | |
| virtual const double | alphaMz () const |
| The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\). More... | |
| virtual const double | alrmoller (const double q2, const double y) const |
| The computation of the parity violating asymmetry in Moller scattering. More... | |
| const double | Als (const double mu, const int Nf_in, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) with \(N_f\) active flavours in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| const double | Als (const double mu, const orders order, const bool Nf_thr, const bool qed_flag) const |
| The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More... | |
| const double | Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const |
| const double | Alstilde5 (const double mu) const |
| The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More... | |
| virtual const double | amuon () const |
| The computation of the anomalous magnetic moment of the muon \(a_\mu=(g_\mu-2)/2\). More... | |
| const double | Beta_e (int nm, unsigned int nf) const |
| QED beta function coefficients - eq. (36) hep-ph/0512066. More... | |
| const double | Beta_s (int nm, unsigned int nf) const |
| QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More... | |
| virtual const double | BrHtobb () const |
| The Br \((H\to b \bar{b})\) in the Standard Model. More... | |
| virtual const double | BrHtocc () const |
| The Br \((H\to c \bar{c})\) in the Standard Model. More... | |
| virtual const double | BrHtogaga () const |
| The Br \((H\to \gamma \gamma)\) in the Standard Model. More... | |
| virtual const double | BrHtogg () const |
| The Br \(\(H\to gg)\) in the Standard Model. More... | |
| virtual const double | BrHtomumu () const |
| The Br \((H\to \mu^+ \mu^-)\) in the Standard Model. More... | |
| virtual const double | BrHtoss () const |
| The Br \((H\to s \bar{s})\) in the Standard Model. More... | |
| virtual const double | BrHtotautau () const |
| The Br \((H\to \tau^+ \tau^-)\) in the Standard Model. More... | |
| virtual const double | BrHtoWWstar () const |
| The Br \((H\to W W^*)\) in the Standard Model. More... | |
| virtual const double | BrHtoZga () const |
| The Br \((H\to Z \gamma)\) in the Standard Model. More... | |
| virtual const double | BrHtoZZstar () const |
| The Br \((H\to Z Z^*)\) in the Standard Model. More... | |
| virtual const double | BrW (const Particle fi, const Particle fj) const |
| The branching ratio of the \(W\) boson decaying into a SM fermion pair, \(Br(W\to f_i f_j)\). More... | |
| const double | c02 () const |
| The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More... | |
| virtual bool | CheckFlags () const |
| A method to check the sanity of the set of model flags. More... | |
| virtual bool | CheckParameters (const std::map< std::string, double > &DPars) |
| A method to check if all the mandatory parameters for StandardModel have been provided in model initialization. More... | |
| bool | checkSMparamsForEWPO () |
| A method to check whether the parameters relevant to the EWPO are updated. More... | |
| const double | computeBrHto4f () const |
| The Br \((H\to 4f)\) in the Standard Model. More... | |
| const double | computeBrHto4l2 () const |
| The Br \((H\to 4l)\) \(l=e,\mu\) in the Standard Model. More... | |
| const double | computeBrHto4l3 () const |
| The Br \((H\to 4l)\) \(l=e,\mu,\tau\) in the Standard Model. More... | |
| const double | computeBrHto4q () const |
| The Br \((H\to 4q)\) in the Standard Model. More... | |
| const double | computeBrHto4v () const |
| The Br \((H\to 4\nu)\) in the Standard Model. More... | |
| const double | computeBrHtobb () const |
| The Br \((H\to bb)\) in the Standard Model. More... | |
| const double | computeBrHtocc () const |
| The Br \((H\to cc)\) in the Standard Model. More... | |
| const double | computeBrHtoevmuv () const |
| The Br \((H\to e \nu \mu \nu)\) in the Standard Model. More... | |
| const double | computeBrHtogaga () const |
| The Br \((H\to\gamma\gamma)\) in the Standard Model. More... | |
| const double | computeBrHtogg () const |
| The Br \((H\to gg)\) in the Standard Model. More... | |
| const double | computeBrHtollvv2 () const |
| The Br \((H\to l^+ l^- \nu \nu)\) \(l=e,\mu\) in the Standard Model. More... | |
| const double | computeBrHtollvv3 () const |
| The Br \((H\to l^+ l^- \nu \nu)\) \(l=e,\mu,\tau\) in the Standard Model. More... | |
| const double | computeBrHtomumu () const |
| The Br \((H\to \mu\mu)\) in the Standard Model. More... | |
| const double | computeBrHtoss () const |
| The Br \((H\to ss)\) in the Standard Model. More... | |
| const double | computeBrHtotautau () const |
| The Br \((H\to \tau\tau)\) in the Standard Model. More... | |
| const double | computeBrHtoWW () const |
| The Br \((H\to WW)\) in the Standard Model. More... | |
| const double | computeBrHtoZga () const |
| The Br \((H\to Z\gamma)\) in the Standard Model. More... | |
| const double | computeBrHtoZZ () const |
| The Br \((H\to ZZ)\) in the Standard Model. More... | |
| void | ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const |
| A method to collect \(\Delta r_{\mathrm{rem}}\) computed via subclasses. More... | |
| void | ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const |
| A method to collect \(\Delta\rho\) computed via subclasses. More... | |
| const double | computeGammaHgaga_tt () const |
| The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| const double | computeGammaHgaga_tW () const |
| The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| const double | computeGammaHgaga_WW () const |
| The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| const double | computeGammaHgg_bb () const |
| The bottom loop contribution to \(H\to gg\) in the Standard Model. More... | |
| const double | computeGammaHgg_tb () const |
| The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More... | |
| const double | computeGammaHgg_tt () const |
| The top loop contribution to \(H\to gg\) in the Standard Model. More... | |
| const double | computeGammaHTotal () const |
| The Higgs total width in the Standard Model. More... | |
| const double | computeGammaHZga_tt () const |
| The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More... | |
| const double | computeGammaHZga_tW () const |
| The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More... | |
| const double | computeGammaHZga_WW () const |
| The \(W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. Currently it returns the value of tab 41 in ref. [Heinemeyer:2013tqa]. More... | |
| const double | computeSigmabbH (const double sqrt_s) const |
| The bbH production cross section in the Standard Model. More... | |
| const double | computeSigmaggH (const double sqrt_s) const |
| The ggH cross section in the Standard Model. More... | |
| const double | computeSigmaggH_bb (const double sqrt_s) const |
| The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More... | |
| const double | computeSigmaggH_tb (const double sqrt_s) const |
| The top-bottom interference contribution to the ggH cross section in the Standard Model. More... | |
| const double | computeSigmaggH_tt (const double sqrt_s) const |
| The square of the top-quark contribution to the ggH cross section in the Standard Model. More... | |
| const double | computeSigmatHq (const double sqrt_s) const |
| The tHq production cross section in the Standard Model. More... | |
| const double | computeSigmattH (const double sqrt_s) const |
| The ttH production cross section in the Standard Model. More... | |
| const double | computeSigmaVBF (const double sqrt_s) const |
| The VBF cross section in the Standard Model. More... | |
| const double | computeSigmaWF (const double sqrt_s) const |
| The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More... | |
| const double | computeSigmaWH (const double sqrt_s) const |
| The WH production cross section in the Standard Model. More... | |
| const double | computeSigmaZF (const double sqrt_s) const |
| The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More... | |
| const double | computeSigmaZH (const double sqrt_s) const |
| The ZH production cross section in the Standard Model. More... | |
| const double | computeSigmaZWF (const double sqrt_s) const |
| The Z W interference fusion contribution \(\sigma_{ZWF}\) to higgs-production cross section in the Standard Model. More... | |
| virtual const double | cW2 () const |
| virtual const double | cW2 (const double Mw_i) const |
| The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More... | |
| virtual const double | Dalpha5hMz () const |
| The 5-quark contribution to the running of the em constant to the \(Z\) pole. \(\Delta\alpha_{had}^{(5)}(M_Z)\). More... | |
| const double | DeltaAlpha () const |
| The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More... | |
| const double | DeltaAlphaL5q () const |
| The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha^{\ell+5q}(M_Z^2)\). More... | |
| const double | DeltaAlphaLepton (const double s) const |
| Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More... | |
| const double | DeltaAlphaTop (const double s) const |
| Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More... | |
| virtual const gslpp::complex | deltaKappaZ_f (const Particle f) const |
| Flavour non-universal vertex corrections to \(\kappa_Z^l\), denoted by \(\Delta\kappa_Z^l\). More... | |
| virtual const double | DeltaR () const |
| The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More... | |
| virtual const double | DeltaRbar () const |
| The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More... | |
| virtual const gslpp::complex | deltaRhoZ_f (const Particle f) const |
| Flavour non-universal vertex corrections to \(\rho_Z^l\), denoted by \(\Delta\rho_Z^l\). More... | |
| virtual const double | eeffAFBbottom (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBcharm (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBe (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBetsub (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBmu (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBstrange (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBtau (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRbottom (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRcharm (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRelectron (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRelectrontsub (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRmuon (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRstrange (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRtau (const double pol_e, const double pol_p, const double s) const |
| const double | eeffsigma (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | eeffsigmaBottom (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaCharm (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaE (const double pol_e, const double pol_p, const double s) const |
| const double | eeffsigmaEbin (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | eeffsigmaEtsub (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaHadron (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaMu (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaStrange (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaTau (const double pol_e, const double pol_p, const double s) const |
| virtual const double | epsilon1 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_1\). More... | |
| virtual const double | epsilon2 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_2\). More... | |
| virtual const double | epsilon3 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_3\). More... | |
| virtual const double | epsilonb () const |
| The SM contribution to the epsilon parameter \(\varepsilon_b\). More... | |
| gslpp::complex | f_triangle (const double tau) const |
| Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | g_triangle (const double tau) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual const gslpp::complex | gA_f (const Particle f) const |
| The effective leptonic neutral-current axial-vector coupling \(g_A^l\) in the SM. More... | |
| virtual const double | Gamma_had () const |
| The hadronic decay width of the \(Z\) boson, \(\Gamma_{h}\). More... | |
| virtual const double | Gamma_inv () const |
| The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More... | |
| virtual const double | Gamma_muon () const |
| The computation of the muon decay. More... | |
| virtual const double | Gamma_tau_l_nunu (const Particle l) const |
| The computation of the leptonic tau decays. More... | |
| virtual const double | Gamma_Z () const |
| The total decay width of the \(Z\) boson, \(\Gamma_Z\). More... | |
| virtual const double | GammaHtobb () const |
| The \(\Gamma(H\to b \bar{b})\) in the Standard Model. More... | |
| virtual const double | GammaHtocc () const |
| The \(\Gamma(H\to c \bar{c})\) in the Standard Model. More... | |
| virtual const double | GammaHtogaga () const |
| The \(\Gamma(H\to \gamma \gamma)\) in the Standard Model. More... | |
| virtual const double | GammaHtogg () const |
| The \(\Gamma(H\to gg)\) in the Standard Model. More... | |
| virtual const double | GammaHtomumu () const |
| The \(\Gamma(H\to \mu^+ \mu^-)\) in the Standard Model. More... | |
| virtual const double | GammaHtoss () const |
| The \(\Gamma(H\to s \bar{s})\) in the Standard Model. More... | |
| virtual const double | GammaHTot () const |
| The total Higgs width \(\Gamma(H)\) in the Standard Model. More... | |
| virtual const double | GammaHtotautau () const |
| The \(\Gamma(H\to \tau^+ \tau^-)\) in the Standard Model. More... | |
| virtual const double | GammaHtoWWstar () const |
| The \(\Gamma(H\to W W^*)\) in the Standard Model. More... | |
| virtual const double | GammaHtoZga () const |
| The \(\Gamma(H\to Z \gamma)\) in the Standard Model. More... | |
| virtual const double | GammaHtoZZstar () const |
| The \(\Gamma(H\to Z Z^*)\) in the Standard Model. More... | |
| virtual const double | GammaW () const |
| The total width of the \(W\) boson, \(\Gamma_W\). More... | |
| virtual const double | GammaW (const Particle fi, const Particle fj) const |
| A partial decay width of the \(W\) boson decay into a SM fermion pair. More... | |
| virtual const double | GammaZ (const Particle f) const |
| The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More... | |
| virtual const double | gAnue () const |
| The effective (muon) neutrino-electron axial-vector coupling: gAnue. More... | |
| const double | getAle () const |
| A get method to retrieve the fine-structure constant \(\alpha\). More... | |
| const double | getAlsMz () const |
| A get method to access the value of \(\alpha_s(M_Z)\). More... | |
| virtual const double | getCBd () const |
| The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More... | |
| virtual const double | getCBs () const |
| The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More... | |
| virtual const double | getCCC1 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual const double | getCCC2 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual const double | getCCC3 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual const double | getCCC4 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual const double | getCCC5 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual const double | getCDMK () const |
| The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More... | |
| virtual const double | getCepsK () const |
| The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More... | |
| const CKM & | getCKM () const |
| A get method to retrieve the member object of type CKM. More... | |
| const double | getDAle5Mz () const |
| A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More... | |
| const double | getDelGammaZ () const |
| A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More... | |
| const double | getDelMw () const |
| A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More... | |
| const double | getDelR0b () const |
| A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| const double | getDelR0c () const |
| A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| const double | getDelR0l () const |
| A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| const double | getDelSigma0H () const |
| A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More... | |
| const double | getDelSin2th_b () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More... | |
| const double | getDelSin2th_l () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More... | |
| const double | getDelSin2th_q () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More... | |
| const std::string | getFlagKappaZ () const |
| A method to retrieve the model flag KappaZ. More... | |
| const std::string | getFlagMw () const |
| A method to retrieve the model flag Mw. More... | |
| const std::string | getFlagRhoZ () const |
| A method to retrieve the model flag RhoZ. More... | |
| const Flavour & | getFlavour () const |
| const double | getGF () const |
| A get method to retrieve the Fermi constant \(G_\mu\). More... | |
| const int | getIterationNo () const |
| const Particle & | getLeptons (const QCD::lepton p) const |
| A get method to retrieve the member object of a lepton. More... | |
| virtual StandardModelMatching & | getMatching () const |
| A get method to access the member reference of type StandardModelMatching. More... | |
| virtual const double | getMHl () const |
| A get method to retrieve the Higgs mass \(m_h\). More... | |
| virtual const double | getmq (const QCD::quark q, const double mu) const |
| The MSbar running quark mass computed at NLO. More... | |
| const double | getMuw () const |
| A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More... | |
| const double | getMw () const |
| A get method to access the input value of the mass of the \(W\) boson \(M_W\). More... | |
| EWSMApproximateFormulae * | getMyApproximateFormulae () const |
| A get method to retrieve the member pointer of type EWSMApproximateFormulae. More... | |
| EWSMcache * | getMyEWSMcache () const |
| A get method to retrieve the member pointer of type EWSMcache. More... | |
| LeptonFlavour * | getMyLeptonFlavour () const |
| EWSMOneLoopEW * | getMyOneLoopEW () const |
| A get method to retrieve the member pointer of type EWSMOneLoopEW,. More... | |
| EWSMThreeLoopEW * | getMyThreeLoopEW () const |
| EWSMThreeLoopEW2QCD * | getMyThreeLoopEW2QCD () const |
| EWSMThreeLoopQCD * | getMyThreeLoopQCD () const |
| EWSMTwoFermionsLEP2 * | getMyTwoFermionsLEP2 () const |
| A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More... | |
| EWSMTwoLoopEW * | getMyTwoLoopEW () const |
| EWSMTwoLoopQCD * | getMyTwoLoopQCD () const |
| const double | getMz () const |
| A get method to access the mass of the \(Z\) boson \(M_Z\). More... | |
| virtual const double | getPhiBd () const |
| Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More... | |
| virtual const double | getPhiBs () const |
| Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More... | |
| virtual const StandardModel & | getTrueSM () const |
| const gslpp::matrix< gslpp::complex > | getUPMNS () const |
| A get method to retrieve the object of the PMNS matrix. More... | |
| const gslpp::matrix< gslpp::complex > | getVCKM () const |
| A get method to retrieve the CKM matrix. More... | |
| const gslpp::matrix< gslpp::complex > & | getYd () const |
| A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYe () const |
| A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYn () const |
| A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYu () const |
| A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More... | |
| virtual const double | gLnuN2 () const |
| The effective neutrino nucleon LH coupling: gLnuN2. More... | |
| virtual const double | gRnuN2 () const |
| The effective neutrino nucleon RH coupling: gRnuN2. More... | |
| virtual const gslpp::complex | gV_f (const Particle f) const |
| The effective leptonic neutral-current vector coupling \(g_V^l\) in the SM. More... | |
| virtual const double | gVnue () const |
| The effective (muon) neutrino-electron vector coupling: gVnue. More... | |
| gslpp::complex | I_triangle_1 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | I_triangle_2 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual bool | Init (const std::map< std::string, double > &DPars) |
| A method to initialize the model parameters. More... | |
| virtual bool | InitializeModel () |
| A method to initialize the model. More... | |
| const double | intMLL2eeeeus2 (const double s, const double t0, const double t1) const |
| const double | intMLR2eeeets2 (const double s, const double t0, const double t1) const |
| const double | intMLRtilde2eeeest2 (const double s, const double t0, const double t1) const |
| const double | intMRR2eeeeus2 (const double s, const double t0, const double t1) const |
| const bool | IsFlagNoApproximateGammaZ () const |
| A method to retrieve the model flag NoApproximateGammaZ. More... | |
| const bool | IsFlagWithoutNonUniversalVC () const |
| A method to retrieve the model flag WithoutNonUniversalVC. More... | |
| const bool | isSMSuccess () const |
| A get method to retrieve the success status of the Standard Model update and matching. More... | |
| virtual const gslpp::complex | kappaZ_f (const Particle f) const |
| The effective leptonic neutral-current coupling \(\kappa_Z^l\) in the SM. More... | |
| virtual const double | LEP2AFBbottom (const double s) const |
| virtual const double | LEP2AFBcharm (const double s) const |
| virtual const double | LEP2AFBe (const double s) const |
| virtual const double | LEP2AFBmu (const double s) const |
| virtual const double | LEP2AFBtau (const double s) const |
| virtual const double | LEP2dsigmadcosBinE (const double s, const double cos, const double cosmin, const double cosmax) const |
| virtual const double | LEP2dsigmadcosBinMu (const double s, const double cos, const double cosmin, const double cosmax) const |
| virtual const double | LEP2dsigmadcosBinTau (const double s, const double cos, const double cosmin, const double cosmax) const |
| virtual const double | LEP2dsigmadcosE (const double s, const double cos) const |
| virtual const double | LEP2dsigmadcosMu (const double s, const double cos) const |
| virtual const double | LEP2dsigmadcosTau (const double s, const double cos) const |
| virtual const double | LEP2Rbottom (const double s) const |
| virtual const double | LEP2Rcharm (const double s) const |
| virtual const double | LEP2sigmaBottom (const double s) const |
| virtual const double | LEP2sigmaCharm (const double s) const |
| virtual const double | LEP2sigmaE (const double s) const |
| virtual const double | LEP2sigmaHadron (const double s) const |
| virtual const double | LEP2sigmaMu (const double s) const |
| virtual const double | LEP2sigmaTau (const double s) const |
| const double | MLL2eeff (const Particle f, const double s, const double t) const |
| const double | MLR2eeff (const Particle f, const double s) const |
| const double | MRL2eeff (const Particle f, const double s) const |
| const double | MRR2eeff (const Particle f, const double s, const double t) const |
| virtual const double | Mw () const |
| The SM prediction for the \(W\)-boson mass in the on-shell scheme, \(M_{W,\mathrm{SM}}\). More... | |
| const double | Mw_tree () const |
| The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More... | |
| const double | MwbarFromMw (const double Mw) const |
| A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More... | |
| const double | MwFromMwbar (const double Mwbar) const |
| A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More... | |
| double | Mzbar () const |
| The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More... | |
| virtual const double | N_nu () const |
| The number of neutrinos obtained indirectly from the measurements at the Z pole, \(N_{\nu}\). More... | |
| virtual bool | PostUpdate () |
| The post-update method for StandardModel. More... | |
| virtual bool | PreUpdate () |
| The pre-update method for StandardModel. More... | |
| virtual const double | Qwemoller (const double q2, const double y) const |
| The computation of the electron's weak charge. More... | |
| virtual const double | Qwn () const |
| The computation of the neutron weak charge: Qwn. More... | |
| virtual const double | Qwp () const |
| The computation of the proton weak charge: Qwp. More... | |
| virtual const double | R0_f (const Particle f) const |
| The ratio \(R_\ell^0=\Gamma(Z\to {\rm hadrons})/\Gamma(Z\to \ell^+ \ell^-)\). More... | |
| virtual const double | R_inv () const |
| The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More... | |
| virtual const double | rho_GammaW (const Particle fi, const Particle fj) const |
| EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More... | |
| virtual const gslpp::complex | rhoZ_f (const Particle f) const |
| The effective leptonic neutral-current coupling \(\rho_Z^l\) in the SM. More... | |
| virtual const double | Ruc () const |
| virtual const double | RWc () const |
| The ratio \(R_{W,c)=\Gamma(W\to c + X)/\Gamma(W\to had)\). More... | |
| virtual const double | RWlilj (const Particle li, const Particle lj) const |
| The lepton universality ratio \(R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)\). More... | |
| virtual const double | RZlilj (const Particle li, const Particle lj) const |
| The lepton universality ratio \(R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)\). More... | |
| const double | s02 () const |
| The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More... | |
| void | setCKM (const CKM &CKMMatrix) |
| A set method to change the CKM matrix. More... | |
| virtual bool | setFlag (const std::string name, const bool value) |
| A method to set a flag of StandardModel. More... | |
| void | setFlagCacheInStandardModel (bool FlagCacheInStandardModel) |
| A set method to change the model flag CacheInStandardModel of StandardModel. More... | |
| void | setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ) |
| bool | setFlagSigmaForAFB (const bool flagSigmaForAFB_i) |
| bool | setFlagSigmaForR (const bool flagSigmaForR_i) |
| virtual bool | setFlagStr (const std::string name, const std::string value) |
| A method to set a flag of StandardModel. More... | |
| void | setRequireCKM (bool requireCKM) |
| A set method to change the value of requireCKM. More... | |
| void | setSMSuccess (bool success) const |
| A set method to change the success status of the Standard Model update and matching. More... | |
| void | setYd (const gslpp::matrix< gslpp::complex > &Yd) |
| A set method to set the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| void | setYe (const gslpp::matrix< gslpp::complex > &Ye) |
| A set method to set the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| void | setYu (const gslpp::matrix< gslpp::complex > &Yu) |
| A set method to set the Yukawa matrix of the up-type quarks, \(Y_u\). More... | |
| virtual const double | sigma0_had () const |
| The hadronic cross section for \(e^+e^- \to Z \to \mathrm{hadrons}\) at the \(Z\)-pole, \(\sigma_h^0\). More... | |
| virtual const double | SigmaeeHee (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to e^+ e^- H)\) in the Standard Model. More... | |
| virtual const double | SigmaeeHvv (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to \nu \bar{\nu} H)\) in the Standard Model. More... | |
| virtual const double | SigmaeeZH (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to Z H)\) in the Standard Model. More... | |
| virtual const double | sin2thetaEff (const Particle f) const |
| The effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\,\ell}\) for \(Z\ell\bar{\ell}\) at the the \(Z\)-mass scale. More... | |
| StandardModel () | |
| The default constructor. More... | |
| const double | sW2 () const |
| virtual const double | sW2 (const double Mw_i) const |
| The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More... | |
| const double | sW2_MSbar_Approx () const |
| The (approximated formula for the) square of the sine of the weak mixing angle in the MSbar scheme, denoted as \(\hat{s}_{W}^2\). See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) More... | |
| const double | sW2_ND () const |
| The square of the sine of the weak mixing angle in the MSbar-ND scheme (w/o decoupling $\alpha\ln(m_t/M_Z)$ terms), denoted as \(\hat{s}_{ND}^2\). See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) (eq. 10.13a/10.13b) More... | |
| virtual const double | TauLFU_gmuge () const |
| The computation of the LFU ratio \(g_\mu/ g_e \). More... | |
| virtual const double | TauLFU_gtauge () const |
| The computation of the LFU ratio \(g_\tau/ g_e \). More... | |
| virtual const double | TauLFU_gtaugmu () const |
| The computation of the LFU ratio \(g_\tau/ g_\mu \). More... | |
| virtual const double | TauLFU_gtaugmuK () const |
| The computation of the LFU ratio \(\left(g_\tau/ g_\mu\right)_K \). More... | |
| virtual const double | TauLFU_gtaugmuPi () const |
| The computation of the LFU ratio \(\left(g_\tau/ g_\mu\right)_\pi \). More... | |
| virtual const double | ThetaLnuN () const |
| The effective neutrino nucleon LH parameter: ThetaLnuN. More... | |
| virtual const double | ThetaRnuN () const |
| The effective neutrino nucleon RH parameter: ThetaRnuN. More... | |
| const double | tovers2 (const double cosmin, const double cosmax) const |
| const double | uovers2 (const double cosmin, const double cosmax) const |
| virtual bool | Update (const std::map< std::string, double > &DPars) |
| The update method for StandardModel. More... | |
| const double | v () const |
| The Higgs vacuum expectation value. More... | |
| virtual | ~StandardModel () |
| The default destructor. More... | |
| Public Member Functions inherited from QCD | |
| const double | AboveTh (const double mu) const |
| The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| void | addParameters (std::vector< std::string > params_i) |
| A method to add parameters that are specific to only one set of observables. More... | |
| const double | Als (const double mu, const int Nf_in, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) with \(N_f\) active flavours in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| const double | Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const |
| const double | Als4 (const double mu) const |
| The value of \(\alpha_s^{\mathrm{FULLNLO}}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\). More... | |
| const double | AlsByOrder (const double mu, const int Nf_in, const orders order=FULLNLO) const |
| const double | AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const |
| const double | AlsOLD (const double mu, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| const double | AlsWithInit (const double mu, const double alsi, const double mu_i, const int nf, const orders order) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) from \(\alpha_s(\mu_i)\) in the \(\overline{\mathrm{MS}}\) scheme, where it is forbidden to across a flavour threshold in the RG running from \(\mu_i\) to \(\mu\). More... | |
| const double | AlsWithLambda (const double mu, const orders order) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme with the use of \(\Lambda_{\rm QCD}\). More... | |
| const double | BelowTh (const double mu) const |
| The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| const double | Beta0 (const double nf) const |
| The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| const double | Beta1 (const double nf) const |
| The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| const double | Beta2 (const double nf) const |
| The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| const double | Beta3 (const double nf) const |
| The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| void | CacheShift (double cache[][5], int n) const |
| A member used to manage the caching for this class. More... | |
| void | CacheShift (int cache[][5], int n) const |
| const orders | FullOrder (orders order) const |
| Return the FULLORDER enum corresponding to order. More... | |
| const double | Gamma0 (const double nf) const |
| The \(\gamma_0\) coefficient used to compute the running of a mass. More... | |
| const double | Gamma1 (const double nf) const |
| The \(\gamma_1\) coefficient used to compute the running of a mass. More... | |
| const double | Gamma2 (const double nf) const |
| The \(\gamma_2\) coefficient used to compute the running of a mass. More... | |
| const double | getAlsM () const |
| A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More... | |
| const BParameter & | getBBd () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More... | |
| const BParameter & | getBBd_subleading () const |
| For getting the subleading bag parameters \(R_2 - R_3\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More... | |
| const BParameter & | getBBs () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More... | |
| const BParameter & | getBBs_subleading () const |
| For getting the subleading bag parameters \(R_2 - R_3\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More... | |
| const BParameter & | getBD () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta c = 2\) process in the \(D^0\) meson system. More... | |
| const BParameter & | getBK () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta s = 2\) process in the \(K^0\) meson system. More... | |
| const BParameter & | getBKd1 () const |
| const BParameter & | getBKd3 () const |
| const double | getCF () const |
| A get method to access the Casimir factor of QCD. More... | |
| const double | getMAls () const |
| A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More... | |
| const Meson & | getMesons (const QCD::meson m) const |
| A get method to access a meson as an object of the type Meson. More... | |
| const double | getMtpole () const |
| A get method to access the pole mass of the top quark. More... | |
| const double | getMub () const |
| A get method to access the threshold between five- and four-flavour theory in GeV. More... | |
| const double | getMuc () const |
| A get method to access the threshold between four- and three-flavour theory in GeV. More... | |
| const double | getMut () const |
| A get method to access the threshold between six- and five-flavour theory in GeV. More... | |
| const double | getNc () const |
| A get method to access the number of colours \(N_c\). More... | |
| const double | getOptionalParameter (std::string name) const |
| A method to get parameters that are specific to only one set of observables. More... | |
| const Particle & | getQuarks (const QCD::quark q) const |
| A get method to access a quark as an object of the type Particle. More... | |
| std::vector< std::string > | getUnknownParameters () |
| A method to get the vector of the parameters that have been specified in the configuration file but not being used. More... | |
| void | initializeBParameter (std::string name_i) const |
| A method to initialize B Parameter and the corresponding meson. More... | |
| void | initializeMeson (QCD::meson meson_i) const |
| A method to initialize a meson. More... | |
| bool | isQCDsuccess () const |
| A getter for the QCDsuccess flag. More... | |
| const double | logLambda (const double nf, orders order) const |
| Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More... | |
| const double | Mbar2Mp (const double mbar, const quark q, const orders order=FULLNNLO) const |
| Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More... | |
| const double | Mofmu2Mbar (const double m, const double mu, const quark q) const |
| Converts a quark running mass at an arbitrary scale to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More... | |
| const double | Mp2Mbar (const double mp, const quark q, orders order=FULLNNLO) const |
| Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More... | |
| const double | Mrun (const double mu, const double m, const quark q, const orders order=FULLNNLO) const |
| Computes a running quark mass \(m(\mu)\) from \(m(m)\). More... | |
| const double | Mrun (const double mu_f, const double mu_i, const double m, const quark q, const orders order=FULLNNLO) const |
| Runs a quark mass from \(\mu_i\) to \(\mu_f\). More... | |
| const double | Mrun4 (const double mu_f, const double mu_i, const double m) const |
| The running of a mass with the number of flavours \(n_f = 4\). More... | |
| const double | MS2DRqmass (const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| const double | MS2DRqmass (const double MSscale, const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| const double | Nf (const double mu) const |
| The number of active flavour at scale \(\mu\). More... | |
| const double | NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const |
| Threshold corrections in matching \(\alpha_s(n_f+1)\) with \(\alpha_s(n_f)\) from eq. (34) of hep-ph/0512060. More... | |
| const std::string | orderToString (const orders order) const |
| Converts an object of the enum type "orders" to the corresponding string. More... | |
| QCD () | |
| Constructor. More... | |
| void | setComputemt (bool computemt) |
| A set method to change the value of computemt. More... | |
| void | setMtpole (double mtpole_in) |
| A method to set the pole mass of the top quark. More... | |
| void | setNc (double Nc) |
| A set method to change the number of colours \(N_c\). More... | |
| void | setOptionalParameter (std::string name, double value) |
| A method to set the parameter value for the parameters that are specific to only one set of observables. More... | |
| void | setQuarkMass (const quark q, const double mass) |
| A set method to change the mass of a quark. More... | |
| const double | Thresholds (const int i) const |
| For accessing the active flavour threshold scales. More... | |
| Public Member Functions inherited from Model | |
| void | addMissingModelParameter (const std::string &missingParameterName) |
| std::vector< std::string > | getmissingModelParameters () |
| unsigned int | getMissingModelParametersCount () |
| std::string | getModelName () const |
| A method to fetch the name of the model. More... | |
| const double & | getModelParam (std::string name) const |
| bool | isModelFWC_DF2 () const |
| bool | isModelGeneralTHDM () const |
| bool | isModelGeorgiMachacek () const |
| bool | IsModelInitialized () const |
| A method to check if the model is initialized. More... | |
| bool | isModelLinearized () const |
| bool | isModelNPquadratic () const |
| bool | isModelParam (std::string name) const |
| bool | isModelSUSY () const |
| bool | isModelTHDM () const |
| bool | isModelTHDMW () const |
| bool | IsUpdateError () const |
| A method to check if there was any error in the model update process. More... | |
| Model () | |
| The default constructor. More... | |
| void | raiseMissingModelParameterCount () |
| void | setModelFWC_DF2 () |
| void | setModelGeneralTHDM () |
| void | setModelGeorgiMachacek () |
| void | setModelInitialized (bool ModelInitialized) |
| A set method to fix the failure or success of the initialization of the model. More... | |
| void | setModelLinearized (bool linearized=true) |
| void | setModelName (const std::string name) |
| A method to set the name of the model. More... | |
| void | setModelNPquadratic (bool NPquadratic=true) |
| void | setModelSUSY () |
| void | setModelTHDM () |
| void | setModelTHDMW () |
| void | setSliced (bool Sliced) |
| void | setUpdateError (bool UpdateError) |
| A set method to fix the update status as success or failure. More... | |
| virtual | ~Model () |
| The default destructor. More... | |
Additional Inherited Members | |
| Public Types inherited from StandardModel | |
| enum | LEP2RCs { Weak = 0 , WeakBox , ISR , QEDFSR , QCDFSR , NUMofLEP2RCs } |
| enum | orders_EW { EW1 = 0 , EW1QCD1 , EW1QCD2 , EW2 , EW2QCD1 , EW3 , orders_EW_size } |
| An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More... | |
| Public Types inherited from QCD | |
| enum | lepton { NEUTRINO_1 , ELECTRON , NEUTRINO_2 , MU , NEUTRINO_3 , TAU , NOLEPTON } |
| An enum type for leptons. More... | |
| enum | meson { P_0 , P_P , K_0 , K_P , D_0 , D_P , D_S , B_D , B_P , B_S , B_C , PHI , K_star , K_star_P , K_S , D_star_P , RHO , RHO_P , OMEGA , MESON_END } |
| An enum type for mesons. More... | |
| enum | quark { UP , DOWN , CHARM , STRANGE , TOP , BOTTOM } |
| An enum type for quarks. More... | |
| Static Public Attributes inherited from StandardModel | |
| static const double | GeVminus2_to_nb = 389379.338 |
| static const double | Mw_error = 0.00001 |
| The target accuracy of the iterative calculation of the \(W\)-boson mass in units of GeV. More... | |
| static const int | NSMvars = 26 |
| The number of the model parameters in StandardModel. More... | |
| static const int | NumSMParamsForEWPO = 33 |
| The number of the SM parameters that are relevant to the EW precision observables. More... | |
| static std::string | SMvars [NSMvars] |
| A string array containing the labels of the model parameters in StandardModel. More... | |
| Static Public Attributes inherited from QCD | |
| static const int | NQCDvars = 11 |
| The number of model parameters in QCD. More... | |
| static std::string | QCDvars [NQCDvars] |
| An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More... | |
| Protected Member Functions inherited from StandardModel | |
| const double | AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| const double | AFB_NoISR_q (const QCD::quark q_flavor, const double s) const |
| bool | checkEWPOscheme (const std::string scheme) const |
| A method to check if a given scheme name in string form is valid. More... | |
| virtual void | computeCKM () |
| The method to compute the CKM matrix. More... | |
| virtual void | computeYukawas () |
| The method to compute the Yukawas matrix. More... | |
| double | Delta_EWQCD (const QCD::quark q) const |
| The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More... | |
| const double | getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm133 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm167 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu130 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu136 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu161 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau130 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau136 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau161 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau207 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom130 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom133 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom136 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom161 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom167 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom172 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom183 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom189 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom192 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom196 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom200 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom202 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom205 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom207 (double x) const |
| const double | getIntegrand_dsigmaBox_charm130 (double x) const |
| const double | getIntegrand_dsigmaBox_charm133 (double x) const |
| const double | getIntegrand_dsigmaBox_charm136 (double x) const |
| const double | getIntegrand_dsigmaBox_charm161 (double x) const |
| const double | getIntegrand_dsigmaBox_charm167 (double x) const |
| const double | getIntegrand_dsigmaBox_charm172 (double x) const |
| const double | getIntegrand_dsigmaBox_charm183 (double x) const |
| const double | getIntegrand_dsigmaBox_charm189 (double x) const |
| const double | getIntegrand_dsigmaBox_charm192 (double x) const |
| const double | getIntegrand_dsigmaBox_charm196 (double x) const |
| const double | getIntegrand_dsigmaBox_charm200 (double x) const |
| const double | getIntegrand_dsigmaBox_charm202 (double x) const |
| const double | getIntegrand_dsigmaBox_charm205 (double x) const |
| const double | getIntegrand_dsigmaBox_charm207 (double x) const |
| const double | getIntegrand_dsigmaBox_down130 (double x) const |
| const double | getIntegrand_dsigmaBox_down133 (double x) const |
| const double | getIntegrand_dsigmaBox_down136 (double x) const |
| const double | getIntegrand_dsigmaBox_down161 (double x) const |
| const double | getIntegrand_dsigmaBox_down167 (double x) const |
| const double | getIntegrand_dsigmaBox_down172 (double x) const |
| const double | getIntegrand_dsigmaBox_down183 (double x) const |
| const double | getIntegrand_dsigmaBox_down189 (double x) const |
| const double | getIntegrand_dsigmaBox_down192 (double x) const |
| const double | getIntegrand_dsigmaBox_down196 (double x) const |
| const double | getIntegrand_dsigmaBox_down200 (double x) const |
| const double | getIntegrand_dsigmaBox_down202 (double x) const |
| const double | getIntegrand_dsigmaBox_down205 (double x) const |
| const double | getIntegrand_dsigmaBox_down207 (double x) const |
| const double | getIntegrand_dsigmaBox_mu130 (double x) const |
| const double | getIntegrand_dsigmaBox_mu133 (double x) const |
| const double | getIntegrand_dsigmaBox_mu136 (double x) const |
| const double | getIntegrand_dsigmaBox_mu161 (double x) const |
| const double | getIntegrand_dsigmaBox_mu167 (double x) const |
| const double | getIntegrand_dsigmaBox_mu172 (double x) const |
| const double | getIntegrand_dsigmaBox_mu183 (double x) const |
| const double | getIntegrand_dsigmaBox_mu189 (double x) const |
| const double | getIntegrand_dsigmaBox_mu192 (double x) const |
| const double | getIntegrand_dsigmaBox_mu196 (double x) const |
| const double | getIntegrand_dsigmaBox_mu200 (double x) const |
| const double | getIntegrand_dsigmaBox_mu202 (double x) const |
| const double | getIntegrand_dsigmaBox_mu205 (double x) const |
| const double | getIntegrand_dsigmaBox_mu207 (double x) const |
| const double | getIntegrand_dsigmaBox_strange130 (double x) const |
| const double | getIntegrand_dsigmaBox_strange133 (double x) const |
| const double | getIntegrand_dsigmaBox_strange136 (double x) const |
| const double | getIntegrand_dsigmaBox_strange161 (double x) const |
| const double | getIntegrand_dsigmaBox_strange167 (double x) const |
| const double | getIntegrand_dsigmaBox_strange172 (double x) const |
| const double | getIntegrand_dsigmaBox_strange183 (double x) const |
| const double | getIntegrand_dsigmaBox_strange189 (double x) const |
| const double | getIntegrand_dsigmaBox_strange192 (double x) const |
| const double | getIntegrand_dsigmaBox_strange196 (double x) const |
| const double | getIntegrand_dsigmaBox_strange200 (double x) const |
| const double | getIntegrand_dsigmaBox_strange202 (double x) const |
| const double | getIntegrand_dsigmaBox_strange205 (double x) const |
| const double | getIntegrand_dsigmaBox_strange207 (double x) const |
| const double | getIntegrand_dsigmaBox_tau130 (double x) const |
| const double | getIntegrand_dsigmaBox_tau133 (double x) const |
| const double | getIntegrand_dsigmaBox_tau136 (double x) const |
| const double | getIntegrand_dsigmaBox_tau161 (double x) const |
| const double | getIntegrand_dsigmaBox_tau167 (double x) const |
| const double | getIntegrand_dsigmaBox_tau172 (double x) const |
| const double | getIntegrand_dsigmaBox_tau183 (double x) const |
| const double | getIntegrand_dsigmaBox_tau189 (double x) const |
| const double | getIntegrand_dsigmaBox_tau192 (double x) const |
| const double | getIntegrand_dsigmaBox_tau196 (double x) const |
| const double | getIntegrand_dsigmaBox_tau200 (double x) const |
| const double | getIntegrand_dsigmaBox_tau202 (double x) const |
| const double | getIntegrand_dsigmaBox_tau205 (double x) const |
| const double | getIntegrand_dsigmaBox_tau207 (double x) const |
| const double | getIntegrand_dsigmaBox_up130 (double x) const |
| const double | getIntegrand_dsigmaBox_up133 (double x) const |
| const double | getIntegrand_dsigmaBox_up136 (double x) const |
| const double | getIntegrand_dsigmaBox_up161 (double x) const |
| const double | getIntegrand_dsigmaBox_up167 (double x) const |
| const double | getIntegrand_dsigmaBox_up172 (double x) const |
| const double | getIntegrand_dsigmaBox_up183 (double x) const |
| const double | getIntegrand_dsigmaBox_up189 (double x) const |
| const double | getIntegrand_dsigmaBox_up192 (double x) const |
| const double | getIntegrand_dsigmaBox_up196 (double x) const |
| const double | getIntegrand_dsigmaBox_up200 (double x) const |
| const double | getIntegrand_dsigmaBox_up202 (double x) const |
| const double | getIntegrand_dsigmaBox_up205 (double x) const |
| const double | getIntegrand_dsigmaBox_up207 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom130 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom133 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom136 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom161 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom167 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom172 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom183 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom189 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom192 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom196 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom200 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom202 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom205 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom207 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm130 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm133 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm136 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm161 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm167 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm172 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm183 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm189 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm192 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm196 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm200 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm202 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm205 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm207 (double x) const |
| const double | getIntegrand_sigmaWithISR_down130 (double x) const |
| const double | getIntegrand_sigmaWithISR_down133 (double x) const |
| const double | getIntegrand_sigmaWithISR_down136 (double x) const |
| const double | getIntegrand_sigmaWithISR_down161 (double x) const |
| const double | getIntegrand_sigmaWithISR_down167 (double x) const |
| const double | getIntegrand_sigmaWithISR_down172 (double x) const |
| const double | getIntegrand_sigmaWithISR_down183 (double x) const |
| const double | getIntegrand_sigmaWithISR_down189 (double x) const |
| const double | getIntegrand_sigmaWithISR_down192 (double x) const |
| const double | getIntegrand_sigmaWithISR_down196 (double x) const |
| const double | getIntegrand_sigmaWithISR_down200 (double x) const |
| const double | getIntegrand_sigmaWithISR_down202 (double x) const |
| const double | getIntegrand_sigmaWithISR_down205 (double x) const |
| const double | getIntegrand_sigmaWithISR_down207 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu130 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu136 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu161 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu172 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu183 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu189 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu192 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu196 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu200 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu202 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu205 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu207 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange130 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange133 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange136 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange161 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange167 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange172 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange183 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange189 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange192 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange196 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange200 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange202 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange205 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange207 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau130 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau136 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau161 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau172 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau183 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau189 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau192 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau196 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau200 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau202 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau205 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau207 (double x) const |
| const double | getIntegrand_sigmaWithISR_up130 (double x) const |
| const double | getIntegrand_sigmaWithISR_up133 (double x) const |
| const double | getIntegrand_sigmaWithISR_up136 (double x) const |
| const double | getIntegrand_sigmaWithISR_up161 (double x) const |
| const double | getIntegrand_sigmaWithISR_up167 (double x) const |
| const double | getIntegrand_sigmaWithISR_up172 (double x) const |
| const double | getIntegrand_sigmaWithISR_up183 (double x) const |
| const double | getIntegrand_sigmaWithISR_up189 (double x) const |
| const double | getIntegrand_sigmaWithISR_up192 (double x) const |
| const double | getIntegrand_sigmaWithISR_up196 (double x) const |
| const double | getIntegrand_sigmaWithISR_up200 (double x) const |
| const double | getIntegrand_sigmaWithISR_up202 (double x) const |
| const double | getIntegrand_sigmaWithISR_up205 (double x) const |
| const double | getIntegrand_sigmaWithISR_up207 (double x) const |
| const double | Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| const double | Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const |
| const double | Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| double | m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const |
| double | RAq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More... | |
| double | resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const |
| A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | RVh () const |
| The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More... | |
| double | RVq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More... | |
| double | SchemeToDouble (const std::string scheme) const |
| A method to convert a given scheme name in string form into a floating-point number with double precision. More... | |
| virtual void | setParameter (const std::string name, const double &value) |
| A method to set the value of a parameter of StandardModel. More... | |
| const double | sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| const double | sigma_NoISR_q (const QCD::quark q_flavor, const double s) const |
| double | taub () const |
| Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More... | |
| Protected Member Functions inherited from QCD | |
| const double | MassOfNf (int nf) const |
| The Mbar mass of the heaviest quark in the theory with Nf active flavour. More... | |
| Protected Attributes inherited from StandardModel | |
| double | A |
| The CKM parameter \(A\) in the Wolfenstein parameterization. More... | |
| double | ale |
| The fine-structure constant \(\alpha\). More... | |
| double | alpha21 |
| double | alpha31 |
| double | AlsMz |
| The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More... | |
| bool | bSigmaForAFB |
| bool | bSigmaForR |
| double | dAl5hMz |
| The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). (Non-input parameter) More... | |
| double | dAle5Mz |
| The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\), used as input for FlagMWinput = FALSE. More... | |
| double | delGammaZ |
| The theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\), in GeV. More... | |
| double | delMw |
| The theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\), in GeV. More... | |
| double | delR0b |
| The theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| double | delR0c |
| The theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| double | delR0l |
| The theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| double | delsigma0H |
| The theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\) in nb. More... | |
| double | delSin2th_b |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More... | |
| double | delSin2th_l |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More... | |
| double | delSin2th_q |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More... | |
| double | delta |
| double | etab |
| The CKM parameter \(\bar{\eta}\) in the Wolfenstein parameterization. More... | |
| bool | flag_order [orders_EW_size] |
| An array of internal flags controlling the inclusions of higher-order corrections. More... | |
| bool | FlagFixMuwMut |
| A boolean for the model flag FixMuwMut. More... | |
| bool | flagLEP2 [NUMofLEP2RCs] |
| double | gamma |
| \(\gamma \) used as an input for FlagWolfenstein = FALSE More... | |
| double | GF |
| The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More... | |
| double | lambda |
| The CKM parameter \(\lambda\) in the Wolfenstein parameterization. More... | |
| Particle | leptons [6] |
| An array of Particle objects for the leptons. More... | |
| double | mHl |
| The Higgs mass \(m_h\) in GeV. More... | |
| double | muw |
| A matching scale \(\mu_W\) around the weak scale in GeV. More... | |
| double | Mw_inp |
| The mass of the \(W\) boson in GeV used as input for FlagMWinput = TRUE. More... | |
| CKM | myCKM |
| An object of type CKM. More... | |
| PMNS | myPMNS |
| double | Mz |
| The mass of the \(Z\) boson in GeV. More... | |
| bool | requireCKM |
| An internal flag to control whether the CKM matrix has to be recomputed. More... | |
| bool | requireYe |
| An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More... | |
| bool | requireYn |
| An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More... | |
| double | rhob |
| The CKM parameter \(\bar{\rho}\) in the Wolfenstein parameterization. More... | |
| double | s12 |
| double | s13 |
| double | s23 |
| Flavour | SMFlavour |
| An object of type Flavour. More... | |
| Matching< StandardModelMatching, StandardModel > | SMM |
| An object of type Matching. More... | |
| double | Vcb |
| \(\vert V_{cb} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| double | Vub |
| \(\vert V_{ub} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| double | Vud |
| \(\vert V_{ud} \vert \) used as an input for FlagWolfenstein = FALSE and FlagUseVud = TRUE More... | |
| double | Vus |
| \(\vert V_{us} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| gslpp::matrix< gslpp::complex > | Yd |
| The Yukawa matrix of the down-type quarks. More... | |
| gslpp::matrix< gslpp::complex > | Ye |
| The Yukawa matrix of the charged leptons. More... | |
| gslpp::matrix< gslpp::complex > | Yn |
| The Yukawa matrix of the neutrinos. More... | |
| gslpp::matrix< gslpp::complex > | Yu |
| The Yukawa matrix of the up-type quarks. More... | |
| Protected Attributes inherited from QCD | |
| double | AlsM |
| The strong coupling constant at the mass scale MAls, \(\alpha_s(M_{\alpha_s})\). More... | |
| double | CA |
| double | CF |
| bool | computemt |
| Switch for computing the \(\overline{\mathrm{MS}}\) mass of the top quark. More... | |
| double | dAdA_NA |
| double | dFdA_NA |
| double | dFdF_NA |
| bool | FlagMpole2MbarNumeric |
| A flag to determine whether the pole mass to \(\over \mathrm{MS}\) mass conversion is done numerically. More... | |
| bool | FlagMtPole |
| A flag to determine whether the pole mass of the top quark is used as input. More... | |
| double | MAls |
| The mass scale in GeV at which the strong coupling measurement is provided. More... | |
| double | mtpole |
| The pole mass of the top quark. More... | |
| double | mub |
| The threshold between five- and four-flavour theory in GeV. More... | |
| double | muc |
| The threshold between four- and three-flavour theory in GeV. More... | |
| double | mut |
| The threshold between six- and five-flavour theory in GeV. More... | |
| double | NA |
| double | Nc |
| The number of colours. More... | |
| bool | QCDsuccess =true |
| Particle | quarks [6] |
| The vector of all SM quarks. More... | |
| bool | requireYd |
| Switch for generating the Yukawa couplings to the down-type quarks. More... | |
| bool | requireYu |
| Switch for generating the Yukawa couplings to the up-type quarks. More... | |
| double | TF |
| Protected Attributes inherited from Model | |
| bool | isSliced = false |
| A boolean set to true if the current istance is a slice of an extended object. More... | |
| std::map< std::string, std::reference_wrapper< const double > > | ModelParamMap |
| bool | UpdateError = false |
| A boolean set to false if update is successful. More... | |
| EWSM_Output::EWSM_Output | ( | const StandardModel & | SM_in | ) |
Constructor.
| [in] | EWSM_in | a reference to an object of type EWSM |
Definition at line 20 of file EWSM_Output.cpp.
| void EWSM_Output::outputEachDeltaKappaZ | ( | const double | f_AlphaToGF, |
| const double | cW2overSW2, | ||
| const double | DeltaRho[StandardModel::orders_EW_size], | ||
| const double | deltaKappa_rem[StandardModel::orders_EW_size], | ||
| const double | DeltaRbar_rem, | ||
| const bool | bool_Zbb, | ||
| const double | taub[StandardModel::orders_EW_size], | ||
| const double | ZbbSubtract, | ||
| const double | Zgamma_EW2 | ||
| ) | const |
Definition at line 583 of file EWSM_Output.cpp.
| void EWSM_Output::outputEachDeltaKappaZ_l | ( | const QCD::lepton | l, |
| const double | Mw_i | ||
| ) | const |
Definition at line 443 of file EWSM_Output.cpp.
| void EWSM_Output::outputEachDeltaKappaZ_q | ( | const QCD::quark | q, |
| const double | Mw_i | ||
| ) | const |
Definition at line 506 of file EWSM_Output.cpp.
| void EWSM_Output::outputEachDeltaR | ( | const double | Mw_i | ) | const |
Definition at line 25 of file EWSM_Output.cpp.
| void EWSM_Output::outputEachDeltaRhoZ | ( | const double | f_AlphaToGF, |
| const double | DeltaRho[StandardModel::orders_EW_size], | ||
| const double | deltaRho_rem[StandardModel::orders_EW_size], | ||
| const double | DeltaRbar_rem, | ||
| const bool | bool_Zbb, | ||
| const double | taub[StandardModel::orders_EW_size], | ||
| const double | ZbbSubtract | ||
| ) | const |
Definition at line 336 of file EWSM_Output.cpp.
| void EWSM_Output::outputEachDeltaRhoZ_l | ( | const QCD::lepton | l, |
| const double | Mw_i | ||
| ) | const |
Definition at line 211 of file EWSM_Output.cpp.
| void EWSM_Output::outputEachDeltaRhoZ_q | ( | const QCD::quark | q, |
| const double | Mw_i | ||
| ) | const |
Definition at line 266 of file EWSM_Output.cpp.
1.9.2 