A model class for new physics in the form the dimension-six effective Lagrangian in the basis of Barbieri and Strumia [27]. More...
#include <NPEffectiveBS.h>
A model class for new physics in the form the dimension-six effective Lagrangian in the basis of Barbieri and Strumia [27].
This is a Model class containing parameters and functions associated with the dimension-six effective Lagrangian:
\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i \]
where only the SM gauge-invariant and flavour-diagonal dimension-six operators that are relevant to the electroweak precision observables are considered:
\begin{align} \mathcal{O}_{WB} &= (H^\dagger\tau^a H) W^a_{\mu\nu}B^{\mu\nu}, & \mathcal{O}_{H} &= | H^\dagger D_\mu H|^2\,, \nonumber\\ \mathcal{O}_{LL} &= \frac{1}{2}(\overline{L}\gamma_\mu\tau^a L)^2\,, & \mathcal{O}^\prime_{HL} &= i(H^\dagger D_\mu\tau^a H)(\overline{L}\gamma^\mu\tau^a L)\,, \nonumber\\ \mathcal{O}^\prime_{HQ} &= i(H^\dagger D_\mu\tau^a H)(\overline{Q}\gamma^\mu\tau^a Q)\,, & \mathcal{O}_{HL} &= i(H^\dagger D_\mu H)(\overline{L}\gamma^\mu L)\,, \nonumber\\ \mathcal{O}_{HQ} &= i(H^\dagger D_\mu H)(\overline{Q}\gamma^\mu Q)\,, & \mathcal{O}_{HE} &= i(H^\dagger D_\mu H)(\overline{E}\gamma^\mu E)\,, \nonumber\\ \mathcal{O}_{HU} &= i(H^\dagger D_\mu H)(\overline{U}\gamma^\mu U)\,, & \mathcal{O}_{HD} &= i(H^\dagger D_\mu H)(\overline{D}\gamma^\mu D)\,, \end{align}
as well as the Hermitian conjugate for operators \(\mathcal{O}^\prime_{HL}\) to \(\mathcal{O}_{HD}\).
After creating an instance of the current class with the constructor NPEffectiveBS(), it is required to call the initialization method InitializeModel(). In the Monte Carlo run, the constructor as well as the initialization method are called in InputParser::ReadParameters().
The model parameters of NPEffectiveBS are summarized below:
| Label | LaTeX symbol | Description |
|---|---|---|
| cWB_NP | \(C_{WB} \) | The coefficient of the operator \(\mathcal{O}_{WB}= \big(H^\dagger\tau^aH\big)W_{\mu\nu}^a B^{\mu\nu}\). |
| cH_NP | \(C_H\) | The coefficient of the operator \(\mathcal{O}_{H}= \big|H^\dagger D_\mu H\big|^2\). |
| cLL_NP | \(C_{LL} \) | The coefficient of the operator \(\mathcal{O}_{LL}=\frac 12 \big(\overline{L}\,\gamma^\mu\tau^a L\big) \big(\overline{L}\,\gamma_\mu\tau^a L\big)\). |
| cHLp_NP | \(C_{HL}^\prime \) | The coefficient of the operator \(\mathcal{O}_{HL}^\prime=i \big(H^\dagger D_\mu\tau^a H\big) \big(\overline{L}\,\gamma^\mu\tau^a L\big)\). |
| cHQp_NP | \(C_{HQ}^\prime \) | The coefficient of the operator \(\mathcal{O}_{HQ}^\prime=i \big(H^\dagger D_\mu\tau^a H\big) \big(\overline{Q}\,\gamma^\mu\tau^a Q\big)\). |
| cHL_NP | \(C_{HL} \) | The coefficient of the operator \(\mathcal{O}_{HL}=i \big(H^\dagger D_\mu H\big) \big(\overline{L}\,\gamma^\mu L\big) \). |
| cHQ_NP | \(C_{HQ} \) | The coefficient of the operator \(\mathcal{O}_{HQ}=i \big(H^\dagger D_\mu H\big) \big(\overline{Q}\,\gamma^\mu Q\big) \). |
| cHE_NP | \(C_{HE} \) | The coefficient of the operator \(\mathcal{O}_{HE}=i \big(H^\dagger D_\mu H\big) \big(\overline{E}\,\gamma^\mu E\big) \). |
| cHU_NP | \(C_{HU} \) | The coefficient of the operator \(\mathcal{O}_{HU}=i \big(H^\dagger D_\mu H\big) \big(\overline{U}\,\gamma^\mu U\big) \). |
| cHD_NP | \(C_{HD} \) | The coefficient of the operator \(\mathcal{O}_{HD}=i \big(H^\dagger D_\mu H\big) \big(\overline{D}\,\gamma^\mu D\big) \). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
The parameters to be used as inputs when lepton or quark universality are not assumed are the following:
| Label | LaTeX symbol | Description |
|---|---|---|
| cWB_NP | \(C_{WB} \) | The coefficient of the operator \({\cal O}_{WB}=\big(H^\dagger\tau^a H\big)W_{\mu\nu}^a B^{\mu\nu}\). |
| cH_NP | \(C_H\) | The coefficient of the operator \({\cal O}_{H}=\big|H^\dagger D_\mu H\big|^2\). |
| cLL_NP | \(C_{LL} \) | The coefficient of the operator \({\cal O}_{LL}=\frac 12\big(\overline{L}\,\gamma^\mu\tau^a L\big) \big(\overline{L}\,\gamma_\mu\tau^a L\big)\). |
| cHL1p_NP, cHL2p_NP, cHL3p_NP | \( C_{HL_i}^\prime \) | The coefficient of the operator \({\cal O}_{HL_i}^\prime =i\big(H^\dagger D_\mu\tau^a H\big) \big(\overline{L_i}\,\gamma^\mu\tau^a L_i\big)\) for \(i=1,2,3\). |
| cHQ1p_NP, cHQ2p_NP, cHQ3p_NP | \( C_{HQ_i}^\prime \) | The coefficient of the operator \({\cal O}_{HQ_i}^\prime =i\big(H^\dagger D_\mu\tau^a H\big) \big(\overline{Q_i}\,\gamma^\mu\tau^a Q_i\big)\) for \(i=1,2,3\). |
| cHL1_NP, cHL2_NP, cHL3_NP | \( C_{HL_i} \) | The coefficient of the operator \({\cal O}_{HL_i} =i\big(H^\dagger D_\mu H\big) \big(\overline{L_i}\,\gamma^\mu L_i\big)\) for \(i=1,2,3\). |
| cHQ1_NP, cHQ2_NP, cHQ3_NP | \( C_{HQ_i} \) | The coefficient of the operator \({\cal O}_{HQ_i} =i\big(H^\dagger D_\mu H\big) \big(\overline{Q_i}\,\gamma^\mu Q_i\big)\) for \(i=1,2,3\). |
| cHE1_NP, cHE2_NP, cHE3_NP | \( C_{HE_i} \) | The coefficient of the operator \({\cal O}_{HE_i} =i\big(H^\dagger D_\mu H\big) \big(\overline{E_i}\,\gamma^\mu E_i\big)\) for \(i=1,2,3\). |
| cHU1_NP, cHU2_NP, cHU3_NP | \( C_{HU_i} \) | The coefficient of the operator \({\cal O}_{HU_i} =i\big(H^\dagger D_\mu H\big) \big(\overline{U_i}\,\gamma^\mu U_i\big)\) for \(i=1,2,3\). |
| cHD1_NP, cHD2_NP, cHD3_NP | \( C_{HD_i} \) | The coefficient of the operator \({\cal O}_{HD_i} =i\big(H^\dagger D_\mu H\big) \big(\overline{D_i}\,\gamma^\mu D_i\big)\) for \(i=1,2,3\). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
There is no model flag in the current class.
Compared to the base class NPbase, the functions for the following quantities are reimplemented in the current class:
and also the get methods getCoeff() to retrieve the value of each coefficient.
Definition at line 268 of file NPEffectiveBS.h.
Public Member Functions | |
| virtual bool | CheckParameters (const std::map< std::string, double > &DPars) |
| A method to check if all the mandatory parameters for the model have been provided in model initialization. More... | |
| virtual double | deltaGA_f (const Particle f) const |
| New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual double | DeltaGF () const |
| New physics contribution to the Fermi constant. More... | |
| virtual double | deltaGV_f (const Particle f) const |
| New physics contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual double | GammaW () const |
| The total width of the \(W\) boson, \(\Gamma_W\). More... | |
| virtual double | Mw_tree () const |
| The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More... | |
| NPEffectiveBS (const bool FlagLeptonUniversal_in=false, const bool FlagQuarkUniversal_in=false) | |
| Constructor. More... | |
| virtual double | obliqueS () const |
| The oblique parameter \(S\). More... | |
| virtual double | obliqueT () const |
| The oblique parameter \(T\). More... | |
| virtual double | obliqueU () const |
| The oblique parameter \(U\). More... | |
| virtual double | v () const |
| The SM Higgs vacuum expectation value \(v\). More... | |
Public Member Functions inherited from NPbase | |
| virtual double | A_f (const Particle f) const |
| The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More... | |
| virtual double | AFB (const Particle f) const |
| The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More... | |
| virtual double | BrHbbRatio () const |
| The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More... | |
| virtual double | BrHccRatio () const |
| The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More... | |
| virtual double | BrHgagaRatio () const |
| The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHggRatio () const |
| The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHtautauRatio () const |
| The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHWWRatio () const |
| The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZgaRatio () const |
| The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZRatio () const |
| The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual double | computeGammaTotalRatio () const |
| The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More... | |
| virtual double | deltaA_f (const Particle f) const |
| The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More... | |
| virtual double | deltaAFB (const Particle f) const |
| The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More... | |
| virtual double | deltaGamma_Z () const |
| The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More... | |
| virtual double | deltaR0_f (const Particle f) const |
| The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\) or \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\), for leptons or quarks, respectively. More... | |
| virtual double | deltaSigmaHadron () const |
| The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More... | |
| virtual double | deltaSin2thetaEff_e () const |
| The new physics contribution to the effective leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More... | |
| virtual gslpp::complex | gA_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual double | Gamma_Z () const |
| The total decay width of the \(Z\) boson, \(\Gamma_Z\). More... | |
| virtual StandardModel | getTrueSM () const |
| A method to return a StandardModel object from NPbase. More... | |
| virtual gslpp::complex | gV_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual gslpp::complex | kappaZ_f (const Particle f) const |
| The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More... | |
| virtual double | mueeZH (const double sqrt_s) const |
| The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muggH (const double sqrt_s) const |
| The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muggHpttH (const double sqrt_s) const |
| The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muttH (const double sqrt_s) const |
| The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muVBF (const double sqrt_s) const |
| The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muVBFpVH (const double sqrt_s) const |
| The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muVH (const double sqrt_s) const |
| The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muWH (const double sqrt_s) const |
| The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muZH (const double sqrt_s) const |
| The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | Mw () const |
| The mass of the \(W\) boson, \(M_W\). More... | |
| NPbase () | |
| The default constructor. More... | |
| virtual bool | PostUpdate () |
| The post-update method for NPbase. More... | |
| virtual double | R0_f (const Particle f) const |
| The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\) or \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\), for leptons or quarks, respectively. More... | |
| virtual gslpp::complex | rhoZ_f (const Particle f) const |
| The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More... | |
| virtual double | sigma0_had () const |
| The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More... | |
| virtual double | sin2thetaEff (const Particle f) const |
| The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More... | |
Public Member Functions inherited from StandardModel | |
| double | ale_OS (const double mu, orders order=FULLNLO) const |
| The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell schem. More... | |
| double | alphaMz () const |
| The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\). More... | |
| 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... | |
| bool | checkSMparamsForEWPO () |
| A method to check whether the parameters relevant to the EWPO are updated. More... | |
| double | computeAlpha () const |
| The CKM angle \(\alpha\). More... | |
| double | computeBeta () const |
| The CKM angle \(\beta\). More... | |
| double | computeBetas () const |
| The CKM angle \(\beta_s\). More... | |
| double | computeBrHtobb () const |
| The Br \((H\to bb)\) in the Standard Model. More... | |
| double | computeBrHtocc () const |
| The Br \((H\to cc)\) in the Standard Model. More... | |
| double | computeBrHtogaga () const |
| The Br \((H\to\gamma\gamma)\) in the Standard Model. More... | |
| double | computeBrHtogg () const |
| The Br \((H\to gg)\) in the Standard Model. More... | |
| double | computeBrHtotautau () const |
| The Br \((H\to \tau\tau)\) in the Standard Model. More... | |
| double | computeBrHtoWW () const |
| The Br \((H\to WW)\) in the Standard Model. More... | |
| double | computeBrHtoZga () const |
| The Br \((H\to Z\gamma)\) in the Standard Model. More... | |
| 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... | |
| double | computeGamma () const |
| The CKM angle \(\gamma\). More... | |
| double | computeGammaHgaga_tt () const |
| The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| double | computeGammaHgaga_tW () const |
| The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| double | computeGammaHgaga_WW () const |
| The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| double | computeGammaHgg_bb () const |
| The bottom loop contribution to \(H\to gg\) in the Standard Model. More... | |
| double | computeGammaHgg_tb () const |
| The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More... | |
| double | computeGammaHgg_tt () const |
| The top loop contribution to \(H\to gg\) in the Standard Model. More... | |
| double | computeGammaHTotal () const |
| The Higgs total width in the Standard Model. More... | |
| double | computeGammaHZga_tt () const |
| The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More... | |
| double | computeGammaHZga_tW () const |
| The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More... | |
| 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. [89]. More... | |
| gslpp::complex | computelamc () const |
| The product of the CKM elements \(V_{cd} V_{cs}^*\). More... | |
| gslpp::complex | computelamc_d () const |
| The product of the CKM elements \(V_{cd} V_{cb}^*\). More... | |
| gslpp::complex | computelamc_s () const |
| The product of the CKM elements \(V_{cs} V_{cb}^*\). More... | |
| gslpp::complex | computelamt () const |
| The product of the CKM elements \(V_{td} V_{ts}^*\). More... | |
| gslpp::complex | computelamt_d () const |
| The product of the CKM elements \(V_{td} V_{tb}^*\). More... | |
| gslpp::complex | computelamt_s () const |
| The product of the CKM elements \(V_{ts} V_{tb}^*\). More... | |
| gslpp::complex | computelamu () const |
| The product of the CKM elements \(V_{ud} V_{us}^*\). More... | |
| gslpp::complex | computelamu_d () const |
| The product of the CKM elements \(V_{ud} V_{ub}^*\). More... | |
| gslpp::complex | computelamu_s () const |
| The product of the CKM elements \(V_{us} V_{ub}^*\). More... | |
| double | computeRb () const |
| \(R_b=|(V_{ud}V_{ub}^*)/(V_{ud}V_{ub}^*)|\). More... | |
| double | computeRt () const |
| \(R_t=|(V_{td} V_{tb}^*)/(V_{cd}V_{cb}^*)|\). More... | |
| double | computeRts () const |
| \(R_{ts}=|(V_{ts}V_{tb}^*)/(V_{cs}V_{cb}^*)|\). More... | |
| double | computeSigmaggH (const double sqrt_s) const |
| The ggH cross section in the Standard Model. More... | |
| 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... | |
| double | computeSigmaggH_tb (const double sqrt_s) const |
| The top-bottom interference contribution to the ggH cross section in the Standard Model. More... | |
| 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... | |
| double | computeSigmattH (const double sqrt_s) const |
| The ttH production cross section in the Standard Model. More... | |
| double | computeSigmaVBF (const double sqrt_s) const |
| The VBF cross section in the Standard Model. More... | |
| double | computeSigmaWF (const double sqrt_s) const |
| The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More... | |
| double | computeSigmaWH (const double sqrt_s) const |
| The WH production cross section in the Standard Model. More... | |
| double | computeSigmaZF (const double sqrt_s) const |
| The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More... | |
| double | computeSigmaZH (const double sqrt_s) const |
| The ZH production cross section in the Standard Model. More... | |
| 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 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 double | cW2 () 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... | |
| 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... | |
| double | DeltaAlphaLepton (const double s) const |
| Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More... | |
| double | DeltaAlphaTop (const double s) const |
| Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More... | |
| virtual 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 double | DeltaR () const |
| The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More... | |
| virtual double | DeltaRbar () const |
| The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More... | |
| virtual 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 double | epsilon1 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_1\). More... | |
| virtual double | epsilon2 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_2\). More... | |
| virtual double | epsilon3 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_3\). More... | |
| virtual double | epsilonb () const |
| The SM contribution to the epsilon parameter \(\varepsilon_b\). More... | |
| virtual double | Gamma_had () const |
| The hadronic decay width of the \(Z\) boson, \(\Gamma_{h}\). More... | |
| virtual double | Gamma_inv () const |
| The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More... | |
| virtual 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 double | GammaZ (const Particle f) const |
| The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More... | |
| double | getA () const |
| A get method to retrieve the CKM element \(A\). More... | |
| double | getAle () const |
| A get method to retrieve the fine-structure constant \(\alpha\). More... | |
| double | getAlsMz () const |
| A get method to access the value of \(\alpha_s(M_Z)\). More... | |
| CKM | getCKM () const |
| A get method to retrieve the member object of type CKM. More... | |
| 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... | |
| double | getDelGammaZ () const |
| A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More... | |
| double | getDelMw () const |
| A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More... | |
| 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... | |
| double | getDeltaMK () const |
| double | getDmk () const |
| double | getEpsK () const |
| double | getEtab () const |
| A get method to retrieve the CKM element \(\bar{\eta}\). More... | |
| std::string | getFlagKappaZ () const |
| A method to retrieve the model flag KappaZ. More... | |
| std::string | getFlagMw () const |
| A method to retrieve the model flag Mw. More... | |
| std::string | getFlagRhoZ () const |
| A method to retrieve the model flag RhoZ. More... | |
| double | getGF () const |
| A get method to retrieve the Fermi constant \(G_\mu\). More... | |
| int | getIterationNo () const |
| double | getKbarEpsK () const |
| double | getLambda () const |
| A get method to retrieve the CKM element \(\lambda\). More... | |
| Particle | getLeptons (const StandardModel::lepton p) const |
| A get method to retrieve the member object of a lepton. More... | |
| double | getMHl () const |
| A get method to retrieve the Higgs mass \(m_h\). More... | |
| double | getMuw () const |
| A get method to retrieve the matching scale \(\mu_W\) around the weak scale. 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... | |
| Flavour * | getMyFlavour () const |
| LeptonFlavour * | getMyLeptonFlavour () const |
| virtual StandardModelMatching * | getMyMatching () const |
| A get method to access the member pointer of type StandardModelMatching. More... | |
| 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 |
| double | getMz () const |
| A get method to access the mass of the \(Z\) boson \(M_Z\). More... | |
| double | getphiEpsK () const |
| double | getRhob () const |
| A get method to retrieve the CKM element \(\bar{\rho}\). More... | |
| double | getSM_M12D () const |
| gslpp::matrix< gslpp::complex > | getUPMNS () const |
| A get method to retrieve the object of the PMNS matrix. More... | |
| gslpp::matrix< gslpp::complex > | getVCKM () const |
| A get method to retrieve the CKM matrix. More... | |
| gslpp::matrix< gslpp::complex > | getYd () const |
| A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| gslpp::matrix< gslpp::complex > | getYe () const |
| A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| gslpp::matrix< gslpp::complex > | getYn () const |
| A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More... | |
| gslpp::matrix< gslpp::complex > | getYu () const |
| A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). 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... | |
| bool | IsFlagNoApproximateGammaZ () const |
| A method to retrieve the model flag NoApproximateGammaZ. More... | |
| bool | IsFlagWithoutNonUniversalVC () const |
| A method to retrieve the model flag WithoutNonUniversalVC. More... | |
| 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... | |
| 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 bool | PreUpdate () |
| The pre-update method for StandardModel. More... | |
| virtual 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... | |
| double | s02 () const |
| The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. 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) |
| virtual bool | setFlagStr (const std::string name, const std::string value) |
| A method to set a flag of StandardModel. More... | |
| StandardModel () | |
| The default constructor. More... | |
| virtual 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... | |
| double | sW2 () const |
| virtual bool | Update (const std::map< std::string, double > &DPars) |
| The update method for StandardModel. More... | |
| virtual | ~StandardModel () |
| The default destructor. More... | |
Public Member Functions inherited from QCD | |
| double | AboveTh (const double mu) const |
| The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| double | Als (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... | |
| 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... | |
| double | AlsWithInit (const double mu, const double alsi, const double mu_i, 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... | |
| 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... | |
| double | BelowTh (const double mu) const |
| The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| double | Beta0 (const double nf) const |
| The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| double | Beta1 (const double nf) const |
| The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| double | Beta2 (const double nf) const |
| The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| double | geta_0A0 () const |
| double | geta_0A0phi () const |
| double | geta_0A1 () const |
| double | geta_0A12 () const |
| double | geta_0A12phi () const |
| double | geta_0A1phi () const |
| double | geta_0T1 () const |
| double | geta_0T1phi () const |
| double | geta_0T2 () const |
| double | geta_0T23 () const |
| double | geta_0T23phi () const |
| double | geta_0T2phi () const |
| double | geta_0V () const |
| double | geta_0Vphi () const |
| double | geta_1A0 () const |
| double | geta_1A0phi () const |
| double | geta_1A1 () const |
| double | geta_1A12 () const |
| double | geta_1A12phi () const |
| double | geta_1A1phi () const |
| double | geta_1T1 () const |
| double | geta_1T1phi () const |
| double | geta_1T2 () const |
| double | geta_1T23 () const |
| double | geta_1T23phi () const |
| double | geta_1T2phi () const |
| double | geta_1V () const |
| double | geta_1Vphi () const |
| double | geta_2A0 () const |
| double | geta_2A0phi () const |
| double | geta_2A1 () const |
| double | geta_2A12 () const |
| double | geta_2A12phi () const |
| double | geta_2A1phi () const |
| double | geta_2T1 () const |
| double | geta_2T1phi () const |
| double | geta_2T2 () const |
| double | geta_2T23 () const |
| double | geta_2T23phi () const |
| double | geta_2T2phi () const |
| double | geta_2V () const |
| double | geta_2Vphi () const |
| double | getAlsM () const |
| A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More... | |
| 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... | |
| 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... | |
| 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... | |
| 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... | |
| BParameter | getBKd1 () const |
| BParameter | getBKd3 () const |
| double | getBLNPcorr () const |
| double | getBr_B_Xcenu () const |
| double | getBr_Kp_munu () const |
| double | getBr_Kp_P0enu () const |
| double | getbsgamma_E0 () const |
| double | getCF () const |
| A get method to access the Casimir factor of QCD. More... | |
| double | getDeltaP_cu () const |
| double | getFKstarp () const |
| double | getGambino_BRsem () const |
| double | getGambino_Mbkin () const |
| double | getGambino_Mcatmuc () const |
| double | getGambino_muG2 () const |
| double | getGambino_mukin () const |
| double | getGambino_mupi2 () const |
| double | getGambino_rhoD3 () const |
| double | getGambino_rhoLS3 () const |
| gslpp::complex | geth_0 () const |
| gslpp::complex | geth_0_1 () const |
| gslpp::complex | geth_0_1_MP () const |
| gslpp::complex | geth_0_2 () const |
| gslpp::complex | geth_0_MP () const |
| gslpp::complex | geth_m () const |
| gslpp::complex | geth_m_1 () const |
| gslpp::complex | geth_m_2 () const |
| gslpp::complex | geth_p () const |
| gslpp::complex | geth_p_1 () const |
| gslpp::complex | geth_p_2 () const |
| double | getIB_Kl () const |
| double | getIB_Kp () const |
| double | getm_fit2_f0 () const |
| double | getm_fit2_fplus () const |
| double | getm_fit2_fT () 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... | |
| Meson | getMesons (const meson m) const |
| A get method to access a meson as an object of the type Meson. More... | |
| double | getMRA0 () const |
| double | getMRA0phi () const |
| double | getMRA1 () const |
| double | getMRA12 () const |
| double | getMRA12phi () const |
| double | getMRA1phi () const |
| double | getMRT1 () const |
| double | getMRT1phi () const |
| double | getMRT2 () const |
| double | getMRT23 () const |
| double | getMRT23phi () const |
| double | getMRT2phi () const |
| double | getMRV () const |
| double | getMRVphi () const |
| double | getMtpole () const |
| A get method to access the pole mass of the top quark. More... | |
| double | getMub () const |
| A get method to access the threshold between five- and four-flavour theory in GeV. More... | |
| double | getMuc () const |
| A get method to access the threshold between four- and three-flavour theory in GeV. More... | |
| double | getMut () const |
| A get method to access the threshold between six- and five-flavour theory in GeV. More... | |
| double | getNc () const |
| A get method to access the number of colours \(N_c\). More... | |
| double | getOmega_eta_etap () const |
| Particle | getQuarks (const quark q) const |
| A get method to access a quark as an object of the type Particle. More... | |
| double | getr_1_fplus () const |
| double | getr_1_fT () const |
| double | getr_2_f0 () const |
| double | getr_2_fplus () const |
| double | getr_2_fT () const |
| double | getReA0_Kd () const |
| double | getReA2_Kd () const |
| double | logLambda (const double nf, orders order) const |
| Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More... | |
| double | Nf (const double mu) const |
| The number of active flavour at scale \(\mu\). More... | |
| std::string | orderToString (const orders order) const |
| Converts an object of the enum type "orders" to the corresponding string. More... | |
| QCD () | |
| Constructor. More... | |
| void | setNc (double Nc) |
| A set method to change the number of colours \(N_c\). More... | |
| double | Thresholds (const int i) const |
| For accessing the active flavour threshold scales. More... | |
Public Member Functions inherited from Model | |
| const double & | getModelParam (std::string name) const |
| bool | IsModelInitialized () const |
| A method to check if the model is initialized. More... | |
| bool | isModelParam (std::string name) const |
| bool | isModelSUSY () const |
| bool | isModelTHDM () const |
| bool | IsUpdateError () const |
| A method to check if there was any error in the model update process. More... | |
| Model () | |
| The default constructor. More... | |
| std::string | ModelName () const |
| A method to fetch the name of the model. More... | |
| void | setModelInitialized (bool ModelInitialized) |
| A set method to fix the failure or success of the initialization of the model. More... | |
| void | setModelName (const std::string name) |
| A method to set the name of the model. More... | |
| void | setModelSUSY () |
| void | setModelTHDM () |
| void | setUpdateError (bool UpdateError) |
| A set method to fix the update status as success or failure. More... | |
| virtual | ~Model () |
| The default destructor. More... | |
Static Public Attributes | |
| static const int | NNPEffectiveBSVars = 30 |
| The number of the model parameters in NPEffectiveBS. More... | |
| static const int | NNPEffectiveBSVars_LFU = 19 |
| The number of the model parameters in NPEffectiveBS with lepton flavour universality. More... | |
| static const int | NNPEffectiveBSVars_LFU_QFU = 11 |
| The number of the model parameters in NPEffectiveBS with lepton and quark flavour universalities. More... | |
| static const int | NNPEffectiveBSVars_QFU = 22 |
| The number of the model parameters in NPEffectiveBS with quark flavour universality. More... | |
| static const std::string | NPEffectiveBSVars [NNPEffectiveBSVars] |
| A string array containing the labels of the model parameters in NPEffectiveBS. More... | |
| static const std::string | NPEffectiveBSVars_LFU [NNPEffectiveBSVars_LFU] |
| A string array containing the labels of the model parameters in NPEffectiveBS with lepton flavour universality. More... | |
| static const std::string | NPEffectiveBSVars_LFU_QFU [NNPEffectiveBSVars_LFU_QFU] |
| A string array containing the labels of the model parameters in NPEffectiveBS with lepton and quark flavour universalities. More... | |
| static const std::string | NPEffectiveBSVars_QFU [NNPEffectiveBSVars_QFU] |
| A string array containing the labels of the model parameters in NPEffectiveBS with quark flavour universality. 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 = 27 |
| The number of the SM parameters that are relevant to the EW precision observables. More... | |
| static const 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 = 186 |
| The number of model parameters in QCD. More... | |
| static const 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 | |
| virtual void | setParameter (const std::string name, const double &value) |
| A method to set the value of a parameter of the model. More... | |
Protected Member Functions inherited from StandardModel | |
| 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 Yukawa matrices. 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... | |
| 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... | |
| double | taub () const |
| Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More... | |
Protected Attributes | |
| double | cH |
| The dimension-6 operator coefficient \(C_{H}\). More... | |
| double | cHD1 |
| The dimension-6 operator coefficient \(C_{HD_1}\). More... | |
| double | cHD2 |
| The dimension-6 operator coefficient \(C_{HD_2}\). More... | |
| double | cHD3 |
| The dimension-6 operator coefficient \(C_{HD_3}\). More... | |
| double | cHE1 |
| The dimension-6 operator coefficient \(C_{HE_1}\). More... | |
| double | cHE2 |
| The dimension-6 operator coefficient \(C_{HE_2}\). More... | |
| double | cHE3 |
| The dimension-6 operator coefficient \(C_{HE_3}\). More... | |
| double | cHL1 |
| The dimension-6 operator coefficient \(C_{HL_1}\). More... | |
| double | cHL1p |
| The dimension-6 operator coefficient \(C_{HL_1}^\prime\). More... | |
| double | cHL2 |
| The dimension-6 operator coefficient \(C_{HL_2}\). More... | |
| double | cHL2p |
| The dimension-6 operator coefficient \(C_{HL_2}^\prime\). More... | |
| double | cHL3 |
| The dimension-6 operator coefficient \(C_{HL_3}\). More... | |
| double | cHL3p |
| The dimension-6 operator coefficient \(C_{HL_3}^\prime\). More... | |
| double | cHQ1 |
| The dimension-6 operator coefficient \(C_{HQ_1}\). More... | |
| double | cHQ1p |
| The dimension-6 operator coefficient \(C_{HQ_1}^\prime\). More... | |
| double | cHQ2 |
| The dimension-6 operator coefficient \(C_{HQ_2}\). More... | |
| double | cHQ2p |
| The dimension-6 operator coefficient \(C_{HQ_2}^\prime\). More... | |
| double | cHQ3 |
| The dimension-6 operator coefficient \(C_{HQ_3}\). More... | |
| double | cHQ3p |
| The dimension-6 operator coefficient \(C_{HQ_3}^\prime\). More... | |
| double | cHU1 |
| The dimension-6 operator coefficient \(C_{HU_1}\). More... | |
| double | cHU2 |
| The dimension-6 operator coefficient \(C_{HU_2}\). More... | |
| double | cHU3 |
| The dimension-6 operator coefficient \(C_{HU_3}\). More... | |
| double | cL1L1 |
| The dimension-6 operator coefficient \(C_{L_1L_1}\). More... | |
| double | cL1L2 |
| The dimension-6 operator coefficient \(C_{L_1L_2}\). More... | |
| double | cL1L3 |
| The dimension-6 operator coefficient \(C_{L_1L_3}\). More... | |
| double | cL2L2 |
| The dimension-6 operator coefficient \(C_{L_2L_2}\). More... | |
| double | cL2L3 |
| The dimension-6 operator coefficient \(C_{L_2L_3}\). More... | |
| double | cL3L3 |
| The dimension-6 operator coefficient \(C_{L_3L_3}\). More... | |
| double | cWB |
| The dimension-6 operator coefficient \(C_{WB}\). More... | |
| double | Lambda_NP |
| The new physics scale \(\Lambda\). More... | |
Protected Attributes inherited from NPbase | |
| StandardModel | trueSM |
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 | AlsMz |
| The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More... | |
| double | dAle5Mz |
| The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). 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 | 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 | DeltaMK |
| double | Dmk |
| double | EpsK |
| 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... | |
| double | GF |
| The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More... | |
| double | KbarEpsK |
| 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... | |
| CKM | myCKM |
| An object of type CKM. More... | |
| double | Mz |
| The mass of the \(Z\) boson in GeV. More... | |
| double | phiEpsK |
| 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 | SM_M12D |
| gslpp::matrix< gslpp::complex > | UPMNS |
| The PMNS matrix. More... | |
| gslpp::matrix< gslpp::complex > | VCKM |
| The CKM matrix. 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 Model | |
| std::map< std::string, boost::reference_wrapper< const double > > | ModelParamMap |
| bool | UpdateError |
| A boolean set to false if update is successful. More... | |
Private Member Functions | |
| double | deltaGL_f_tmp (const Particle f) const |
| New physics contribution to \(g_L^f\). More... | |
| double | deltaGR_f_tmp (const Particle f) const |
| New physics contribution to \(g_R^f\). More... | |
Private Attributes | |
| const bool | FlagLeptonUniversal |
| An internal boolean flag that is true if assuming lepton flavour universality. More... | |
| const bool | FlagQuarkUniversal |
| An internal boolean flag that is true if assuming quark flavour universality. More... | |
Additional Inherited Members | |
Public Types inherited from StandardModel | |
| enum | lepton { NEUTRINO_1, ELECTRON, NEUTRINO_2, MU, NEUTRINO_3, TAU } |
| An enum type for leptons. More... | |
| 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 | meson { P_0, P_P, K_0, K_P, D_0, B_D, B_P, B_S, PHI, K_star, MESON_END } |
| An enum type for mesons. More... | |
| enum | quark { UP, DOWN, CHARM, STRANGE, TOP, BOTTOM } |
| An enum type for quarks. More... | |
| NPEffectiveBS::NPEffectiveBS | ( | const bool | FlagLeptonUniversal_in = false, |
| const bool | FlagQuarkUniversal_in = false |
||
| ) |
Constructor.
| [in] | FlagLeptonUniversal_in | an internal boolean flag that is true if assuming lepton flavour universality |
| [in] | FlagQuarkUniversal_in | an internal boolean flag that is true if assuming quark flavour universality |
Definition at line 31 of file NPEffectiveBS.cpp.
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virtual |
A method to check if all the mandatory parameters for the model have been provided in model initialization.
| [in] | DPars | a map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant) |
Reimplemented from StandardModel.
Definition at line 184 of file NPEffectiveBS.cpp.
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virtual |
New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).
New physics contribution to the neutral-current axial-vector coupling \(g_A^f\) is given by
\[ \delta g_A^f = \delta g_L^f - \delta g_R^f. \]
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 304 of file NPEffectiveBS.cpp.
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virtual |
New physics contribution to the Fermi constant.
The new physics contribution \(\Delta G\) is defined as
\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]
where \(G_\mu\) is the experimentl value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM. The dimension-six operators yield the following corrections:
\[ \Delta G = - C_{LL}\left(\frac{v}{\Lambda}\right)^2 + C^\prime_{HL_1}\left(\frac{v}{\Lambda}\right)^2 + C^\prime_{HL_2}\left(\frac{v}{\Lambda}\right)^2. \]
See [58] and references therein.
Reimplemented from NPbase.
Definition at line 244 of file NPEffectiveBS.cpp.
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private |
New physics contribution to \(g_L^f\).
New physics contributions to the neutral-current left-handed coupling \(g_L^f\): e.g.,
\[ \delta g_L^{\nu_i} = \frac{C_{HL_i}^\prime-C_{HL_i}}{2} \left(\frac{v}{\Lambda}\right)^2, \qquad \delta g_L^{e_i} = -\frac{C_{HL_i}^\prime+C_{HL_i}}{2} \left(\frac{v}{\Lambda}\right)^2, \]
where \(L\to Q\), \(\nu_i\to u_i\) and \(e_i\to d_i\) for quarks. See [58] and references therein.
| [in] | f | a lepton or quark |
Definition at line 312 of file NPEffectiveBS.cpp.
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private |
New physics contribution to \(g_R^f\).
New physics contributions to the neutral-current right-handed coupling \(g_R^f\): e.g.,
\[ \delta g_R^{e_i} = -\frac{C_{HE_i}}{2} \left(\frac{v}{\Lambda}\right)^2. \]
See [58] and references therein.
| [in] | f | a lepton or quark |
Definition at line 342 of file NPEffectiveBS.cpp.
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virtual |
New physics contribution to the neutral-current vector coupling \(g_V^f\).
New physics contribution to the neutral-current vector coupling \(g_V^f\) is given by
\[ \delta g_V^f = \delta g_L^f + \delta g_R^f. \]
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 299 of file NPEffectiveBS.cpp.
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virtual |
The total width of the \(W\) boson, \(\Gamma_W\).
The width of the \(W\) boson receives the corrections from the operators \(\mathcal{O}^\prime_{HL}\) and \(\mathcal{O}^\prime_{HQ}\), in addition to the corrections via \(S\), \(T\), \(U\) and \(\Delta G\):
\[ \Gamma_W = \Gamma_{W,\mathrm{SM}} \left[ 1 - \frac{3\alpha(M_Z^2)}{4(c_W^2-s_W^2)} \left( S - 2c_W^2\,T - \frac{c_W^2-s_W^2}{2s_W^2}\,U \right) - \frac{1+c_W^2}{2(c_W^2-s_W^2)}\, \Delta G + \left( C_{HL_1}^\prime + C_{HL_2}^\prime + C_{HL_3}^\prime + C_{HQ_1}^\prime + C_{HQ_2}^\prime\right) \left(\frac{v}{\Lambda}\right)^2 \right]. \]
See [58] and references therein.
Reimplemented from NPbase.
Definition at line 254 of file NPEffectiveBS.cpp.
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virtual |
The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\).
The tree-level mass is obtained by subtracting the effect of \(\Delta G\).
Reimplemented from StandardModel.
Definition at line 237 of file NPEffectiveBS.cpp.
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virtual |
The oblique parameter \(S\).
The operator \(\mathcal{O}_{WB}\) contributes to the \(S\) parameter:
\[ S = \frac{4s_Wc_W\, C_{WB} }{\alpha(M_Z^2)} \left(\frac{v}{\Lambda}\right)^2. \]
See [58] and references therein.
Reimplemented from NPbase.
Definition at line 275 of file NPEffectiveBS.cpp.
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virtual |
The oblique parameter \(T\).
The operator \(\mathcal{O}_{H}\) contributes to the \(T\) parameter:
\[ T = - \frac{C_H}{2\alpha(M_Z^2)}\left(\frac{v}{\Lambda}\right)^2. \]
See [58] and references therein.
Reimplemented from NPbase.
Definition at line 284 of file NPEffectiveBS.cpp.
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virtual |
The oblique parameter \(U\).
Reimplemented from NPbase.
Definition at line 291 of file NPEffectiveBS.cpp.
|
protectedvirtual |
A method to set the value of a parameter of the model.
| [in] | name | name of a model parameter |
| [in] | value | the value to be assigned to the parameter specified by name |
Reimplemented from StandardModel.
Definition at line 83 of file NPEffectiveBS.cpp.
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virtual |
The SM Higgs vacuum expectation value \(v\).
\[ v = \left(\frac{1}{\sqrt{2} G_F}\right)^{1/2}. \]
Reimplemented from StandardModel.
Definition at line 228 of file NPEffectiveBS.cpp.
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protected |
The dimension-6 operator coefficient \(C_{H}\).
Definition at line 474 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HD_1}\).
Definition at line 499 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HD_2}\).
Definition at line 500 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HD_3}\).
Definition at line 501 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HE_1}\).
Definition at line 493 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HE_2}\).
Definition at line 494 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HE_3}\).
Definition at line 495 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HL_1}\).
Definition at line 487 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HL_1}^\prime\).
Definition at line 481 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HL_2}\).
Definition at line 488 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HL_2}^\prime\).
Definition at line 482 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HL_3}\).
Definition at line 489 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HL_3}^\prime\).
Definition at line 483 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HQ_1}\).
Definition at line 490 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HQ_1}^\prime\).
Definition at line 484 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HQ_2}\).
Definition at line 491 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HQ_2}^\prime\).
Definition at line 485 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HQ_3}\).
Definition at line 492 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HQ_3}^\prime\).
Definition at line 486 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HU_1}\).
Definition at line 496 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HU_2}\).
Definition at line 497 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{HU_3}\).
Definition at line 498 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{L_1L_1}\).
Definition at line 475 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{L_1L_2}\).
Definition at line 476 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{L_1L_3}\).
Definition at line 477 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{L_2L_2}\).
Definition at line 478 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{L_2L_3}\).
Definition at line 479 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{L_3L_3}\).
Definition at line 480 of file NPEffectiveBS.h.
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protected |
The dimension-6 operator coefficient \(C_{WB}\).
Definition at line 473 of file NPEffectiveBS.h.
|
private |
An internal boolean flag that is true if assuming lepton flavour universality.
Definition at line 511 of file NPEffectiveBS.h.
|
private |
An internal boolean flag that is true if assuming quark flavour universality.
Definition at line 517 of file NPEffectiveBS.h.
|
protected |
The new physics scale \(\Lambda\).
Definition at line 502 of file NPEffectiveBS.h.
|
static |
The number of the model parameters in NPEffectiveBS.
Definition at line 274 of file NPEffectiveBS.h.
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static |
The number of the model parameters in NPEffectiveBS with lepton flavour universality.
Definition at line 280 of file NPEffectiveBS.h.
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static |
The number of the model parameters in NPEffectiveBS with lepton and quark flavour universalities.
Definition at line 292 of file NPEffectiveBS.h.
|
static |
The number of the model parameters in NPEffectiveBS with quark flavour universality.
Definition at line 286 of file NPEffectiveBS.h.
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static |
A string array containing the labels of the model parameters in NPEffectiveBS.
Definition at line 298 of file NPEffectiveBS.h.
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static |
A string array containing the labels of the model parameters in NPEffectiveBS with lepton flavour universality.
Definition at line 304 of file NPEffectiveBS.h.
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static |
A string array containing the labels of the model parameters in NPEffectiveBS with lepton and quark flavour universalities.
Definition at line 316 of file NPEffectiveBS.h.
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static |
A string array containing the labels of the model parameters in NPEffectiveBS with quark flavour universality.
Definition at line 310 of file NPEffectiveBS.h.