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 model class for new physics in the form of the dimension-six effective Lagrangian. More...
#include <NPEffectiveGIMRprime.h>
Inheritance diagram for NPEffectiveGIMRprime:A model class for new physics in the form of the dimension-six effective Lagrangian.
This is a Model class containing parameters and functions associated with the general dimension-six effective Lagrangian. (Use the model name "NPEffectiveGIMRprime_LFU_QFU" to asumme lepton and quark flavour universality)
In this class we consider the dimension-six effective Lagrangian
\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i \]
as written in the basis of [132] , replacing the operators \({\cal O}_{HWB}=\big(H^\dagger\tau^a H\big)W_{\mu\nu}^a B^{\mu\nu}\) and \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\) by \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\) and \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \tau^a D^\nu H\big) W_{\mu\nu}^a\). In this way only 8 dimension 6 operators contribute to electroweak precision observables, the maximum number that can be constrained by the data.
After creating an instance of the current class with the constructor NPEffectiveGIMR(), 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 NPEffectiveGIMR are summarized below:
| Label | LaTeX symbol | Description |
|---|---|---|
| CG | \(C_{G} \) | The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\). |
| CW | \(C_{W} \) | The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\). |
| CHG | \(C_{HG} \) | The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\). |
| CHW | \(C_{HW} \) | The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\). |
| CHB | \(C_{HB} \) | The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\). |
| CDHB | \(C_{DHB} \) | The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\). |
| CDHW | \(C_{DHW}\) | The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \tau^a D^\nu H\big) W_{\mu\nu}^a\). |
| CHbox | \(C_{H\Box}\) | The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\). |
| CH | \(C_{H}\) | The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\). |
| CHL1_kk, CHL1_klr, CHL1_kli | \( (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)\), for \(i,j=1,2,3\). |
| CHL3_kk, CHL3_klr, CHL3_kli | \( (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \tau^a L^j\big)\), for \(i,j=1,2,3\). |
| CHe_kk, CHe_klr, CHe_kli | \( (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)\), for \(i,j=1,2,3\). |
| CHQ1_kk, CHQ1_klr, CHQ1_kli | \( (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\), for \(i,j=1,2,3\). |
| CHQ3_kk, CHQ3_klr, CHQ3_kli | \( (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \tau^a Q^j\big)\), for \(i,j=1,2,3\). |
| CHu_kk, CHu_klr, CHu_kli | \( (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)\), for \(i,j=1,2,3\). |
| CHd_kk, CHd_klr, CHd_kli | \( (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\). |
| CHud_klr, CHud_kli | \(\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\). |
| CeH_klr, CeH_kli | \(\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)\), for \(i,j=1,2,3\). |
| CuH_klr, CuH_kli | \(\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)\), for \(i,j=1,2,3\). |
| CdH_klr, CdH_kli | \(\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)\), for \(i,j=1,2,3\). |
| CuG_klr, CuG_kli | \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\). |
| CuW_klr, CuW_kli | \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \tau_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CuB_klr, CuB_kli | \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CLL_1221, CLL_2112 | \((C_{LL})_{1221,2112}\) | The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\). |
| CLQ1 | \(C_{LQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| CLQ3 | \(C_{LQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \tau_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \tau_a Q^l\big)\). |
| Cee | \(C_{EE}\) | The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Ceu | \(C_{EU}\) | The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| Ced | \(C_{ED}\) | The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CLe | \(C_{LE}\) | The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| CLu | \(C_{LU}\) | The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| CLd | \(C_{LD}\) | The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CQe | \(C_{QE}\) | The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
| eVBFE_i | \(\varepsilon_{VBF}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the VBF production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HAA}, g_{HWW}^{(1,2,3)}, g_{Hgg}, g_{HZuu,HZdd}^{L,R}, g_{HWud}^{L}, g_{Zuu,Zdd}^{L,R}, g_{Wud}^{L})\) |
| eWHE_i | \(\varepsilon_{WH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the WH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{HWW}^{(1,2,3)}, g_{HWud}^{L}, g_{Wud}^{L})\) |
| eZHE_i | \(\varepsilon_{ZH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ZH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HZuu,HZdd}^{L,R}, g_{Zuu,Zdd}^{L,R})\) |
| ettHE_i | \(\varepsilon_{ttH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ttH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{Htt}, g_{Hgg})\) |
Where the hermitian derivatives are defined as
\[ H^\dagger i \overset{\leftrightarrow}{D}_\mu H\equiv H^\dagger i(D_\mu - \overset{\leftarrow}{D}_\mu)H \]
and
\[ H^\dagger i \overset{\leftrightarrow}{D^a_\mu} H\equiv H^\dagger i (\tau^a D_\mu - \overset{\leftarrow}{D}_\mu \tau^a)H. \]
Alternatively, when using the model name "NPEffectiveGIMRprime_LFU_QFU", where lepton and quark flavour universality are assumed, the parameters to be used as inputs for the dimension six coefficients are the following:
| Label | LaTeX symbol | Description |
|---|---|---|
| CG | \(C_{G} \) | The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\). |
| CW | \(C_{W} \) | The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\). |
| CHG | \(C_{HG} \) | The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\). |
| CHW | \(C_{HW} \) | The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\). |
| CHB | \(C_{HB} \) | The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\). |
| CDHB | \(C_{DHB} \) | The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\). |
| CDHW | \(C_{DHW}\) | The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \tau^a D^\nu H\big) W_{\mu\nu}^a\). |
| CHbox | \(C_{H\Box}\) | The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\). |
| CH | \(C_{H}\) | The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\). |
| CHL1 | \( (C_{HL}^{(1)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^i\big)\) (flavor universal). |
| CHL3 | \( (C_{HL}^{(3)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \tau^a L^i\big)\) (flavor universal). |
| CHe | \( (C_{He})_{ii} \) | The coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^i\big)\) (flavor universal). |
| CHQ1 | \( (C_{HQ}^{(1)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^i\big)\) (flavor universal). |
| CHQ3 | \( (C_{HQ}^{(3)})_{ii}\) | The coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \tau^a Q^i\big)\) (flavor universal). |
| CHu | \( (C_{Hu})_{ii} \) | The coefficient of the operator \(({\cal O}_{Hu})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^i\big)\) (flavor universal). |
| CHd | \( (C_{Hd})_{ii} \) | The coefficient of the operator \(({\cal O}_{Hd})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^i\big)\) (flavor universal). |
| CHud_r, CHud_i | \(\mbox{Re}\big[(C_{Hud})_{ii}\big], \mbox{Im}\big[(C_{Hud})_{ii}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ii} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^i\big)\) (flavor universal). |
| CeH_r, CeH_i | \(\mbox{Re}\big[(C_{eH})_{ii}\big], \mbox{Im}\big[(C_{eH})_{ii}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{ii} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^i\big)\) (flavor universal). |
| CuH_r, CuH_i | \(\mbox{Re}\big[(C_{uH})_{ii}\big], \mbox{Im}\big[(C_{uH})_{ii}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{ii} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^i\big)\) (flavor universal). |
| CdH_r, CdH_i | \(\mbox{Re}\big[(C_{dH})_{ii}\big], \mbox{Im}\big[(C_{dH})_{ii}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{ii} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^i\big)\) (flavor universal). |
| CuG_klr, CuG_kli | \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\). |
| CuW_klr, CuW_kli | \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \tau_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CuB_klr, CuB_kli | \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CLL | \((C_{LL})_{1221,2112}\) | The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\). |
| CLQ1 | \(C_{LQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| CLQ3 | \(C_{LQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \tau_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \tau_a Q^l\big)\). |
| Cee | \(C_{EE}\) | The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Ceu | \(C_{EU}\) | The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| Ced | \(C_{ED}\) | The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CLe | \(C_{LE}\) | The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| CLu | \(C_{LU}\) | The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| CLd | \(C_{LD}\) | The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CQe | \(C_{QE}\) | The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
(The parameters associated to the theoretical uncertainties, \(\varepsilon_{X}^i(E)\), are the same for both "NPEffectiveGIMRprime" and "NPEffectiveGIMRprime_LFU_QFU".)
Finally, if the flag MwInput (see below) is set to TRUE, one must also specify the input value for the W mass via the following parameter (Warning: The W width is not implemented in this case):
| Label | LaTeX symbol | Description |
|---|---|---|
| MwInput | \(M_{W} \) | The input value for the W mass in GeV. |
The Flags of NPEffectiveGIMRprime are summarized below:
| Label | Value | Description |
|---|---|---|
| MwInput | TRUE / FALSE | This flag is set to TRUE if the W mass is taken as an input parameter. (Warning: The W width is not implemented in this case.) The default value is FALSE. |
| QuadraticTerms | TRUE / FALSE | This flag is set to TRUE if the quadratic terms in Higgs cross sections and widths are switched on. The default value is FALSE; new physics contributions are linearized. |
See the base classes of the current class.
Definition at line 615 of file NPEffectiveGIMRprime.h.
Public Member Functions | |
| 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... | |
| 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 | BrHmumuRatio () const |
| The ratio of the Br \((H\to \mu^+\mu^-)\) 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 bool | CheckParameters (const std::map< std::string, double > &DPars) |
| A method to check if all the mandatory parameters for NPEffectiveGIMRprime have been provided in model initialization. More... | |
| virtual double | computeGammaTotalRatio () const |
| The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More... | |
| virtual double | deltaG1_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More... | |
| virtual double | deltaG1_hZA () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual double | deltaG1_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More... | |
| virtual double | deltaG2_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More... | |
| virtual double | deltaG2_hZA () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More... | |
| virtual double | deltaG2_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More... | |
| virtual double | deltaG3_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More... | |
| virtual double | deltaG3_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More... | |
| double | deltag3G () const |
| The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More... | |
| gslpp::complex | deltaG_Aff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| gslpp::complex | deltaG_Gff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual double | deltaG_hAA () const |
| The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More... | |
| gslpp::complex | deltaG_hAff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual gslpp::complex | deltaG_hff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More... | |
| gslpp::complex | deltaG_hGff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual double | deltaG_hgg () const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More... | |
| gslpp::complex | deltaG_hZff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| gslpp::complex | deltaG_Zff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual double | deltaGA_f (const Particle p) const |
| New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| double | deltaGammaHbbRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHbbRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHccRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHccRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHgagaRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHgagaRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHggRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More... | |
| double | deltaGammaHggRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHmumuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHmumuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHtautauRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHtautauRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWWRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWWRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZgaRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZgaRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| virtual double | deltaGammaTotalRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More... | |
| virtual double | deltaGammaTotalRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More... | |
| virtual double | DeltaGF () const |
| New physics contribution to the Fermi constant. More... | |
| double | deltaGL_f (const Particle p) const |
| New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More... | |
| virtual gslpp::complex | deltaGL_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| gslpp::complex | deltaGL_Wffh (const Particle pbar, const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| double | deltaGL_Zffh (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| double | deltaGR_f (const Particle p) const |
| New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More... | |
| virtual gslpp::complex | deltaGR_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| gslpp::complex | deltaGR_Wffh (const Particle pbar, const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| double | deltaGR_Zffh (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| virtual double | deltaGV_f (const Particle p) const |
| New physics contribution to the neutral-current vector coupling \(g_V^f\). 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... | |
| double | GammaHbbRatio () const |
| The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More... | |
| double | GammaHccRatio () const |
| The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More... | |
| double | GammaHgagaRatio () const |
| The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| double | GammaHggRatio () const |
| The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More... | |
| double | GammaHmumuRatio () const |
| The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. More... | |
| double | GammaHtautauRatio () const |
| The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More... | |
| double | GammaHWWRatio () const |
| The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More... | |
| double | GammaHZgaRatio () const |
| The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZRatio () const |
| The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual double | GammaW () const |
| The total width of the \(W\) boson, \(\Gamma_W\). More... | |
| virtual double | mueettH (const double sqrt_s) const |
| The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeWBF (const double sqrt_s) const |
| The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. 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... | |
| NPEffectiveGIMRprime (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 bool | PostUpdate () |
| The post-update method for NPEffectiveGIMRprime. More... | |
| virtual bool | setFlag (const std::string name, const bool value) |
| A method to set a flag of NPEffectiveGIMRprime. 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 | aPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More... | |
| virtual double | AuxObs_NP1 () const |
| Auxiliary observable AuxObs_NP1. More... | |
| virtual double | AuxObs_NP10 () const |
| Auxiliary observable AuxObs_NP10. More... | |
| virtual double | AuxObs_NP11 () const |
| Auxiliary observable AuxObs_NP11. More... | |
| virtual double | AuxObs_NP12 () const |
| Auxiliary observable AuxObs_NP12. More... | |
| virtual double | AuxObs_NP13 () const |
| Auxiliary observable AuxObs_NP13. More... | |
| virtual double | AuxObs_NP14 () const |
| Auxiliary observable AuxObs_NP14. More... | |
| virtual double | AuxObs_NP15 () const |
| Auxiliary observable AuxObs_NP15. More... | |
| virtual double | AuxObs_NP16 () const |
| Auxiliary observable AuxObs_NP16. More... | |
| virtual double | AuxObs_NP17 () const |
| Auxiliary observable AuxObs_NP17. More... | |
| virtual double | AuxObs_NP18 () const |
| Auxiliary observable AuxObs_NP18. More... | |
| virtual double | AuxObs_NP19 () const |
| Auxiliary observable AuxObs_NP19. More... | |
| virtual double | AuxObs_NP2 () const |
| Auxiliary observable AuxObs_NP2. More... | |
| virtual double | AuxObs_NP20 () const |
| Auxiliary observable AuxObs_NP20. More... | |
| virtual double | AuxObs_NP3 () const |
| Auxiliary observable AuxObs_NP3. More... | |
| virtual double | AuxObs_NP4 () const |
| Auxiliary observable AuxObs_NP4. More... | |
| virtual double | AuxObs_NP5 () const |
| Auxiliary observable AuxObs_NP5. More... | |
| virtual double | AuxObs_NP6 () const |
| Auxiliary observable AuxObs_NP6. More... | |
| virtual double | AuxObs_NP7 () const |
| Auxiliary observable AuxObs_NP7. More... | |
| virtual double | AuxObs_NP8 () const |
| Auxiliary observable AuxObs_NP8. More... | |
| virtual double | AuxObs_NP9 () const |
| Auxiliary observable AuxObs_NP9. More... | |
| virtual double | bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More... | |
| virtual double | Br_H_exo () const |
| The branching ratio of the of the Higgs into exotic particles. More... | |
| virtual double | Br_H_inv () const |
| The branching ratio of the of the Higgs into invisible particles. More... | |
| virtual double | Br_H_inv_NP () const |
| The branching ratio of the of the Higgs into invisible particles (only invisible new particles). More... | |
| virtual double | BR_Zf (const Particle f) const |
| The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More... | |
| virtual double | BrHtoinvRatio () const |
| The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHvisRatio () const |
| The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHWlvRatio () const |
| The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHWW2l2vRatio () const |
| The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZgaeeRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZgallRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZgamumuRatio () const |
| The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZllRatio () const |
| The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ2e2muRatio () const |
| The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4eRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4lRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4muRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More... | |
| virtual double | cbminuscc () const |
| virtual double | cbminusctau () const |
| virtual double | ccminusctau () const |
| virtual double | cgaga_HB () const |
| The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | cgaplusct () const |
| virtual double | cgg_HB () const |
| The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | cggEff_HB () const |
| The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) More... | |
| virtual double | cgminuscga () const |
| virtual double | cgplusct () const |
| virtual double | cVpluscb () const |
| virtual double | cVplusctau () const |
| virtual double | cZBox_HB () const |
| The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | cZga_HB () const |
| The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | cZZ_HB () const |
| The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) 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 | deltacZ_HB () const |
| The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | deltaG1_hZARatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual double | deltag1ZNP () const |
| The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More... | |
| virtual double | deltag1ZNPEff () const |
| The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More... | |
| virtual double | deltaG_hAARatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual double | deltaG_hggRatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual double | deltaG_hhhRatio () const |
| The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More... | |
| virtual double | deltaGamma_W () const |
| The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More... | |
| virtual double | deltaGamma_Wff (const Particle fi, const Particle fj) const |
| The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). 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 | deltaGamma_Zf (const Particle f) const |
| The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| virtual double | deltaGamma_Zhad () const |
| The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\). More... | |
| virtual double | deltaKgammaNP () const |
| The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More... | |
| virtual double | deltaKgammaNPEff () const |
| The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More... | |
| virtual double | deltaN_nu () const |
| The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More... | |
| virtual double | deltaR0_f (const Particle f) const |
| The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More... | |
| virtual double | deltaR_inv () const |
| The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). 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 electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More... | |
| virtual double | deltaSin2thetaEff_mu () const |
| The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More... | |
| virtual double | deltayb_HB () const |
| The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | deltayc_HB () const |
| The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | deltaymu_HB () const |
| The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | deltayt_HB () const |
| The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | deltaytau_HB () const |
| The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | dxseeWWdcos (const double sqrt_s, const double cos) const |
| The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More... | |
| virtual double | dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const |
| The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. 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_had () const |
| The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\). More... | |
| virtual double | Gamma_Z () const |
| The total decay width of the \(Z\) boson, \(\Gamma_Z\). More... | |
| virtual double | Gamma_Zf (const Particle f) const |
| The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). 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 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 double | kappaAeff () const |
| The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More... | |
| virtual double | kappabeff () const |
| The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More... | |
| virtual double | kappaceff () const |
| The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More... | |
| virtual double | kappaGeff () const |
| The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More... | |
| virtual double | kappamueff () const |
| The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More... | |
| virtual double | kappataueff () const |
| The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More... | |
| virtual double | kappaWeff () const |
| The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). 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 | kappaZAeff () const |
| The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More... | |
| virtual double | kappaZeff () const |
| The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More... | |
| virtual double | lambdaZNP () const |
| The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More... | |
| virtual double | lambz_HB () const |
| The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual double | mueeHvv (const double sqrt_s) const |
| The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeHvvPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueettHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeWBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeWW (const double sqrt_s) const |
| The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeWWPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZBF (const double sqrt_s) const |
| The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) 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 | mueeZllH (const double sqrt_s) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZqqH (const double sqrt_s) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muepWBF (const double sqrt_s) const |
| The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muepZBF (const double sqrt_s) const |
| The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muggHbb (const double sqrt_s) const |
| virtual double | muggHgaga (const double sqrt_s) const |
| virtual double | muggHgagaInt (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More... | |
| virtual double | muggHH (const double sqrt_s) const |
| The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muggHmumu (const double sqrt_s) const |
| virtual double | muggHtautau (const double sqrt_s) const |
| virtual double | muggHWW (const double sqrt_s) const |
| virtual double | muggHWW2l2v (const double sqrt_s) const |
| virtual double | muggHZga (const double sqrt_s) const |
| virtual double | muggHZZ (const double sqrt_s) const |
| virtual double | muggHZZ4l (const double sqrt_s) const |
| virtual double | mummH (const double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muppHmumu (const double sqrt_s) const |
| virtual double | muppHZga (const double sqrt_s) const |
| virtual double | mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const |
| The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class. More... | |
| virtual double | mutHq (const double sqrt_s) const |
| The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHbb (const double sqrt_s) const |
| virtual double | muTHUggHgaga (const double sqrt_s) const |
| virtual double | muTHUggHmumu (const double sqrt_s) const |
| virtual double | muTHUggHtautau (const double sqrt_s) const |
| virtual double | muTHUggHWW (const double sqrt_s) const |
| virtual double | muTHUggHWW2l2v (const double sqrt_s) const |
| virtual double | muTHUggHZga (const double sqrt_s) const |
| virtual double | muTHUggHZgamumu (const double sqrt_s) const |
| virtual double | muTHUggHZZ (const double sqrt_s) const |
| virtual double | muTHUggHZZ4l (const double sqrt_s) const |
| virtual double | muTHUggHZZ4mu (const double sqrt_s) const |
| virtual double | muTHUttHbb (const double sqrt_s) const |
| virtual double | muTHUttHgaga (const double sqrt_s) const |
| virtual double | muTHUttHmumu (const double sqrt_s) const |
| virtual double | muTHUttHtautau (const double sqrt_s) const |
| virtual double | muTHUttHWW (const double sqrt_s) const |
| virtual double | muTHUttHWW2l2v (const double sqrt_s) const |
| virtual double | muTHUttHZga (const double sqrt_s) const |
| virtual double | muTHUttHZZ (const double sqrt_s) const |
| virtual double | muTHUttHZZ4l (const double sqrt_s) const |
| virtual double | muTHUVBFBRinv (const double sqrt_s) const |
| virtual double | muTHUVBFHbb (const double sqrt_s) const |
| virtual double | muTHUVBFHgaga (const double sqrt_s) const |
| virtual double | muTHUVBFHinv (const double sqrt_s) const |
| virtual double | muTHUVBFHmumu (const double sqrt_s) const |
| virtual double | muTHUVBFHtautau (const double sqrt_s) const |
| virtual double | muTHUVBFHWW (const double sqrt_s) const |
| virtual double | muTHUVBFHWW2l2v (const double sqrt_s) const |
| virtual double | muTHUVBFHZga (const double sqrt_s) const |
| virtual double | muTHUVBFHZZ (const double sqrt_s) const |
| virtual double | muTHUVBFHZZ4l (const double sqrt_s) const |
| virtual double | muTHUVHbb (const double sqrt_s) const |
| virtual double | muTHUVHBRinv (const double sqrt_s) const |
| virtual double | muTHUVHgaga (const double sqrt_s) const |
| virtual double | muTHUVHinv (const double sqrt_s) const |
| virtual double | muTHUVHmumu (const double sqrt_s) const |
| virtual double | muTHUVHtautau (const double sqrt_s) const |
| virtual double | muTHUVHWW (const double sqrt_s) const |
| virtual double | muTHUVHWW2l2v (const double sqrt_s) const |
| virtual double | muTHUVHZga (const double sqrt_s) const |
| virtual double | muTHUVHZZ (const double sqrt_s) const |
| virtual double | muTHUVHZZ4l (const double sqrt_s) const |
| virtual double | muTHUWHbb (const double sqrt_s) const |
| virtual double | muTHUWHgaga (const double sqrt_s) const |
| virtual double | muTHUWHmumu (const double sqrt_s) const |
| virtual double | muTHUWHtautau (const double sqrt_s) const |
| virtual double | muTHUWHWW (const double sqrt_s) const |
| virtual double | muTHUWHWW2l2v (const double sqrt_s) const |
| virtual double | muTHUWHZga (const double sqrt_s) const |
| virtual double | muTHUWHZZ (const double sqrt_s) const |
| virtual double | muTHUWHZZ4l (const double sqrt_s) const |
| virtual double | muTHUZHbb (const double sqrt_s) const |
| virtual double | muTHUZHgaga (const double sqrt_s) const |
| virtual double | muTHUZHmumu (const double sqrt_s) const |
| virtual double | muTHUZHtautau (const double sqrt_s) const |
| virtual double | muTHUZHWW (const double sqrt_s) const |
| virtual double | muTHUZHWW2l2v (const double sqrt_s) const |
| virtual double | muTHUZHZga (const double sqrt_s) const |
| virtual double | muTHUZHZZ (const double sqrt_s) const |
| virtual double | muTHUZHZZ4l (const double sqrt_s) const |
| virtual double | muttHbb (const double sqrt_s) const |
| virtual double | muttHgaga (const double sqrt_s) const |
| virtual double | muttHmumu (const double sqrt_s) const |
| virtual double | muttHtautau (const double sqrt_s) const |
| virtual double | muttHWW (const double sqrt_s) const |
| virtual double | muttHWW2l2v (const double sqrt_s) const |
| virtual double | muttHZbbboost (const double sqrt_s) const |
| The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More... | |
| virtual double | muttHZga (const double sqrt_s) const |
| virtual double | muttHZZ (const double sqrt_s) const |
| virtual double | muttHZZ4l (const double sqrt_s) const |
| virtual double | muVBFgamma (const double sqrt_s) const |
| The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More... | |
| virtual double | muVBFHbb (const double sqrt_s) const |
| virtual double | muVBFHgaga (const double sqrt_s) const |
| virtual double | muVBFHmumu (const double sqrt_s) const |
| virtual double | muVBFHtautau (const double sqrt_s) const |
| virtual double | muVBFHWW (const double sqrt_s) const |
| virtual double | muVBFHWW2l2v (const double sqrt_s) const |
| virtual double | muVBFHZga (const double sqrt_s) const |
| virtual double | muVBFHZZ (const double sqrt_s) const |
| virtual double | muVBFHZZ4l (const double sqrt_s) const |
| virtual double | muVHbb (const double sqrt_s) const |
| virtual double | muVHgaga (const double sqrt_s) const |
| virtual double | muVHmumu (const double sqrt_s) const |
| virtual double | muVHtautau (const double sqrt_s) const |
| virtual double | muVHWW (const double sqrt_s) const |
| virtual double | muVHWW2l2v (const double sqrt_s) const |
| virtual double | muVHZga (const double sqrt_s) const |
| virtual double | muVHZZ (const double sqrt_s) const |
| virtual double | muVHZZ4l (const double sqrt_s) const |
| virtual double | muWHbb (const double sqrt_s) const |
| virtual double | muWHgaga (const double sqrt_s) const |
| virtual double | muWHmumu (const double sqrt_s) const |
| virtual double | muWHtautau (const double sqrt_s) const |
| virtual double | muWHWW (const double sqrt_s) const |
| virtual double | muWHWW2l2v (const double sqrt_s) const |
| virtual double | muWHZga (const double sqrt_s) const |
| virtual double | muWHZZ (const double sqrt_s) const |
| virtual double | muWHZZ4l (const double sqrt_s) const |
| virtual double | muZHbb (const double sqrt_s) const |
| virtual double | muZHgaga (const double sqrt_s) const |
| virtual double | muZHmumu (const double sqrt_s) const |
| virtual double | muZHtautau (const double sqrt_s) const |
| virtual double | muZHWW (const double sqrt_s) const |
| virtual double | muZHWW2l2v (const double sqrt_s) const |
| virtual double | muZHZga (const double sqrt_s) const |
| virtual double | muZHZZ (const double sqrt_s) const |
| virtual double | muZHZZ4l (const double sqrt_s) const |
| virtual double | N_nu () const |
| The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More... | |
| NPbase () | |
| The default constructor. More... | |
| virtual double | obliqueW () const |
| The oblique parameter \(W\). More... | |
| virtual double | obliqueY () const |
| The oblique parameter \(Y\). More... | |
| virtual double | ppZHprobe (const double sqrt_s) const |
| The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class. More... | |
| virtual double | R0_f (const Particle f) const |
| The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More... | |
| virtual double | R_inv () const |
| The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). 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... | |
| virtual double | STXS_ggH0j (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH1j_pTH_0_60 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH1j_pTH_120_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH1j_pTH_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH1j_pTH_60_120 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH2j_pTH_0_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH2j_pTH_0_60 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH2j_pTH_120_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH2j_pTH_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH2j_pTH_60_120 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_qqHll_pTV_0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual double | STXS_qqHll_pTV_150_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual double | STXS_qqHll_pTV_150_250_0j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual double | STXS_qqHll_pTV_150_250_1j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual double | STXS_qqHll_pTV_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual double | STXS_qqHlv_pTV_0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual double | STXS_qqHlv_pTV_0_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual double | STXS_qqHlv_pTV_150_250_0j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual double | STXS_qqHlv_pTV_150_250_1j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual double | STXS_qqHlv_pTV_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual double | STXS_qqHqq_pTj_200 (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_qqHqq_Rest (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_qqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_qqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_qqHqq_VBFtopo_Rest (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_qqHqq_VHtopo (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_ttHtH (const double sqrt_s) const |
| The STXS bin \( ttH + tH \). More... | |
| virtual double | STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual double | STXS_WHqqHqq_Rest (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual double | STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual double | STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual double | STXS_WHqqHqq_VH2j (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual double | STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual double | STXS_ZHqqHqq_Rest (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual double | STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual double | STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual double | STXS_ZHqqHqq_VH2j (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual bool | Update (const std::map< std::string, double > &DPars) |
| The update method for NPbase. More... | |
| virtual double | UpperLimitZgammaA (const double sqrt_s) const |
| virtual double | UpperLimitZgammaA13 (const double sqrt_s) const |
| virtual double | UpperLimitZgammaC (const double sqrt_s) const |
| virtual double | UpperLimitZgammaC13 (const double sqrt_s) const |
| virtual double | xseeWW (const double sqrt_s) const |
| Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More... | |
| Public Member Functions inherited from StandardModel | |
| double | Ale (double mu, orders order, bool Nf_thr=true) const |
| The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More... | |
| double | ale_OS (const double mu, orders order=FULLNLO) const |
| The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. 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 | Als (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const |
| The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More... | |
| double | AlsByOrder (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) 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... | |
| double | Beta_e (int nm, unsigned int nf) const |
| QED beta function coefficients - eq. (36) hep-ph/0512066. More... | |
| double | Beta_s (int nm, unsigned int nf) const |
| QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. 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 | 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 | computeBrHtomumu () const |
| The Br \((H\to \mu\mu)\) in the Standard Model. More... | |
| double | computeBrHtoss () const |
| The Br \((H\to ss)\) 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... | |
| double | computeBrHtoZZinv () const |
| The Br \((H\to ZZ \to inv)\) 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 | 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. [138]. 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 |
| 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... | |
| 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_inv () const |
| The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More... | |
| virtual double | GammaZ (const Particle f) const |
| The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). 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... | |
| virtual double | getCBd () const |
| The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More... | |
| virtual double | getCBs () const |
| The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More... | |
| virtual double | getCCC1 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual double | getCCC2 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual double | getCCC3 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual double | getCCC4 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual double | getCCC5 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual double | getCDMK () const |
| The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More... | |
| virtual double | getCepsK () const |
| The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. 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 | getDelR0b () const |
| A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| double | getDelR0c () const |
| A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| double | getDelR0l () const |
| A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| double | getDelSigma0H () const |
| A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More... | |
| 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... | |
| 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 | 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... | |
| 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... | |
| const Flavour & | getFlavour () const |
| double | getGF () const |
| A get method to retrieve the Fermi constant \(G_\mu\). More... | |
| int | getIterationNo () 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 double | getMHl () const |
| A get method to retrieve the Higgs mass \(m_h\). More... | |
| virtual double | getmq (const QCD::quark q, const double mu) const |
| 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... | |
| 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 |
| double | getMz () const |
| A get method to access the mass of the \(Z\) boson \(M_Z\). More... | |
| virtual double | getPhiBd () const |
| Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More... | |
| virtual double | getPhiBs () const |
| Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More... | |
| 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... | |
| virtual double | LEP2AFBbottom (const double s) const |
| virtual double | LEP2AFBcharm (const double s) const |
| virtual double | LEP2AFBmu (const double s) const |
| virtual double | LEP2AFBtau (const double s) const |
| virtual double | LEP2Rbottom (const double s) const |
| virtual double | LEP2Rcharm (const double s) const |
| virtual double | LEP2sigmaBottom (const double s) const |
| virtual double | LEP2sigmaCharm (const double s) const |
| virtual double | LEP2sigmaHadron (const double s) const |
| virtual double | LEP2sigmaMu (const double s) const |
| virtual double | LEP2sigmaTau (const double s) const |
| virtual double | Mw_tree () const |
| The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). 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... | |
| 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... | |
| StandardModel () | |
| The default constructor. More... | |
| double | sW2 () const |
| 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... | |
| virtual double | v () const |
| The Higgs vacuum expectation value. 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... | |
| void | addParameters (std::vector< std::string > params_i) |
| A method to add parameters that are specific to only one set of observables. More... | |
| virtual double | Als (const double mu, const orders order=FULLNLO, bool Nf_thr=true) 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... | |
| virtual double | AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) 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... | |
| 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 | 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 |
| orders | FullOrder (orders order) const |
| Return the FULLORDER enum corresponding to order. More... | |
| double | Gamma0 (const double nf) const |
| The \(\gamma_0\) coefficient used to compute the running of a mass. More... | |
| double | Gamma1 (const double nf) const |
| The \(\gamma_1\) coefficient used to compute the running of a mass. More... | |
| double | Gamma2 (const double nf) const |
| The \(\gamma_2\) coefficient used to compute the running of a mass. More... | |
| 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 | getCF () const |
| A get method to access the Casimir factor of QCD. More... | |
| 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 QCD::meson m) const |
| A get method to access a meson as an object of the type Meson. More... | |
| 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 | getOptionalParameter (std::string name) const |
| A method to get parameters that are specific to only one set of observables. More... | |
| 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... | |
| double | logLambda (const double nf, orders order) const |
| Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More... | |
| double | Mbar2Mp (const double mbar, const orders order=FULLNNLO) const |
| Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More... | |
| double | Mp2Mbar (const double mp, const orders order=FULLNNLO) const |
| Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More... | |
| double | Mrun (const double mu, const double m, const orders order=FULLNNLO) const |
| Computes a running quark mass \(m(\mu)\) from \(m(m)\). More... | |
| double | Mrun (const double mu_f, const double mu_i, const double m, const orders order=FULLNNLO) const |
| Runs a quark mass from \(\mu_i\) to \(\mu_f\). More... | |
| 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... | |
| double | MS2DRqmass (const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| 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... | |
| double | Nf (const double mu) const |
| The number of active flavour at scale \(\mu\). More... | |
| 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... | |
| 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... | |
| 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... | |
| 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 | 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 | 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... | |
Static Public Attributes | |
| static const int | NNPEffectiveGIMRprimeVars = 247 |
| The number of the model parameters in NPEffectiveGIMRprime. More... | |
| static const int | NNPEffectiveGIMRprimeVars_LFU_QFU = 121 |
| The number of the model parameters in NPEffectiveGIMRprime with lepton and quark flavour universalities. More... | |
| static const std::string | NPEffectiveGIMRprimeVars [NNPEffectiveGIMRprimeVars] |
| A string array containing the labels of the model parameters in NPEffectiveGIMRprime if the model flag FlagRotateCHWCHB=false. More... | |
| static const std::string | NPEffectiveGIMRprimeVars_LFU_QFU [NNPEffectiveGIMRprimeVars_LFU_QFU] |
| A string array containing the labels of the model parameters in NPEffectiveGIMRprime with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false. More... | |
| static const std::string | NPEffectiveGIMRprimeVarsRot [NNPEffectiveGIMRprimeVars] |
| A string array containing the labels of the model parameters in NPEffectiveGIMRprime if the model flag FlagRotateCHWCHB=true. More... | |
| static const std::string | NPEffectiveGIMRprimeVarsRot_LFU_QFU [NNPEffectiveGIMRprimeVars_LFU_QFU] |
| A string array containing the labels of the model parameters in NPEffectiveGIMRprime with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true. 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 | |
| gslpp::complex | CfB_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f. More... | |
| gslpp::complex | CfG_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f. More... | |
| gslpp::complex | CfH_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f. More... | |
| gslpp::complex | CfW_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f. More... | |
| double | CHF1_diag (const Particle F) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F. More... | |
| double | CHF3_diag (const Particle F) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F. More... | |
| double | CHf_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f. More... | |
| gslpp::complex | CHud_diag (const Particle u) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HUD}\) corresponding to particle f. More... | |
| 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 | |
| double | AFB_NoISR_l (const QCD::lepton l_flavor, const double s) 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 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 | getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm133 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm167 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm207 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu130 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu136 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu161 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu207 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau130 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau136 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau161 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau207 (double x) const |
| double | getIntegrand_dsigmaBox_bottom130 (double x) const |
| double | getIntegrand_dsigmaBox_bottom133 (double x) const |
| double | getIntegrand_dsigmaBox_bottom136 (double x) const |
| double | getIntegrand_dsigmaBox_bottom161 (double x) const |
| double | getIntegrand_dsigmaBox_bottom167 (double x) const |
| double | getIntegrand_dsigmaBox_bottom172 (double x) const |
| double | getIntegrand_dsigmaBox_bottom183 (double x) const |
| double | getIntegrand_dsigmaBox_bottom189 (double x) const |
| double | getIntegrand_dsigmaBox_bottom192 (double x) const |
| double | getIntegrand_dsigmaBox_bottom196 (double x) const |
| double | getIntegrand_dsigmaBox_bottom200 (double x) const |
| double | getIntegrand_dsigmaBox_bottom202 (double x) const |
| double | getIntegrand_dsigmaBox_bottom205 (double x) const |
| double | getIntegrand_dsigmaBox_bottom207 (double x) const |
| double | getIntegrand_dsigmaBox_charm130 (double x) const |
| double | getIntegrand_dsigmaBox_charm133 (double x) const |
| double | getIntegrand_dsigmaBox_charm136 (double x) const |
| double | getIntegrand_dsigmaBox_charm161 (double x) const |
| double | getIntegrand_dsigmaBox_charm167 (double x) const |
| double | getIntegrand_dsigmaBox_charm172 (double x) const |
| double | getIntegrand_dsigmaBox_charm183 (double x) const |
| double | getIntegrand_dsigmaBox_charm189 (double x) const |
| double | getIntegrand_dsigmaBox_charm192 (double x) const |
| double | getIntegrand_dsigmaBox_charm196 (double x) const |
| double | getIntegrand_dsigmaBox_charm200 (double x) const |
| double | getIntegrand_dsigmaBox_charm202 (double x) const |
| double | getIntegrand_dsigmaBox_charm205 (double x) const |
| double | getIntegrand_dsigmaBox_charm207 (double x) const |
| double | getIntegrand_dsigmaBox_down130 (double x) const |
| double | getIntegrand_dsigmaBox_down133 (double x) const |
| double | getIntegrand_dsigmaBox_down136 (double x) const |
| double | getIntegrand_dsigmaBox_down161 (double x) const |
| double | getIntegrand_dsigmaBox_down167 (double x) const |
| double | getIntegrand_dsigmaBox_down172 (double x) const |
| double | getIntegrand_dsigmaBox_down183 (double x) const |
| double | getIntegrand_dsigmaBox_down189 (double x) const |
| double | getIntegrand_dsigmaBox_down192 (double x) const |
| double | getIntegrand_dsigmaBox_down196 (double x) const |
| double | getIntegrand_dsigmaBox_down200 (double x) const |
| double | getIntegrand_dsigmaBox_down202 (double x) const |
| double | getIntegrand_dsigmaBox_down205 (double x) const |
| double | getIntegrand_dsigmaBox_down207 (double x) const |
| double | getIntegrand_dsigmaBox_mu130 (double x) const |
| double | getIntegrand_dsigmaBox_mu133 (double x) const |
| double | getIntegrand_dsigmaBox_mu136 (double x) const |
| double | getIntegrand_dsigmaBox_mu161 (double x) const |
| double | getIntegrand_dsigmaBox_mu167 (double x) const |
| double | getIntegrand_dsigmaBox_mu172 (double x) const |
| double | getIntegrand_dsigmaBox_mu183 (double x) const |
| double | getIntegrand_dsigmaBox_mu189 (double x) const |
| double | getIntegrand_dsigmaBox_mu192 (double x) const |
| double | getIntegrand_dsigmaBox_mu196 (double x) const |
| double | getIntegrand_dsigmaBox_mu200 (double x) const |
| double | getIntegrand_dsigmaBox_mu202 (double x) const |
| double | getIntegrand_dsigmaBox_mu205 (double x) const |
| double | getIntegrand_dsigmaBox_mu207 (double x) const |
| double | getIntegrand_dsigmaBox_strange130 (double x) const |
| double | getIntegrand_dsigmaBox_strange133 (double x) const |
| double | getIntegrand_dsigmaBox_strange136 (double x) const |
| double | getIntegrand_dsigmaBox_strange161 (double x) const |
| double | getIntegrand_dsigmaBox_strange167 (double x) const |
| double | getIntegrand_dsigmaBox_strange172 (double x) const |
| double | getIntegrand_dsigmaBox_strange183 (double x) const |
| double | getIntegrand_dsigmaBox_strange189 (double x) const |
| double | getIntegrand_dsigmaBox_strange192 (double x) const |
| double | getIntegrand_dsigmaBox_strange196 (double x) const |
| double | getIntegrand_dsigmaBox_strange200 (double x) const |
| double | getIntegrand_dsigmaBox_strange202 (double x) const |
| double | getIntegrand_dsigmaBox_strange205 (double x) const |
| double | getIntegrand_dsigmaBox_strange207 (double x) const |
| double | getIntegrand_dsigmaBox_tau130 (double x) const |
| double | getIntegrand_dsigmaBox_tau133 (double x) const |
| double | getIntegrand_dsigmaBox_tau136 (double x) const |
| double | getIntegrand_dsigmaBox_tau161 (double x) const |
| double | getIntegrand_dsigmaBox_tau167 (double x) const |
| double | getIntegrand_dsigmaBox_tau172 (double x) const |
| double | getIntegrand_dsigmaBox_tau183 (double x) const |
| double | getIntegrand_dsigmaBox_tau189 (double x) const |
| double | getIntegrand_dsigmaBox_tau192 (double x) const |
| double | getIntegrand_dsigmaBox_tau196 (double x) const |
| double | getIntegrand_dsigmaBox_tau200 (double x) const |
| double | getIntegrand_dsigmaBox_tau202 (double x) const |
| double | getIntegrand_dsigmaBox_tau205 (double x) const |
| double | getIntegrand_dsigmaBox_tau207 (double x) const |
| double | getIntegrand_dsigmaBox_up130 (double x) const |
| double | getIntegrand_dsigmaBox_up133 (double x) const |
| double | getIntegrand_dsigmaBox_up136 (double x) const |
| double | getIntegrand_dsigmaBox_up161 (double x) const |
| double | getIntegrand_dsigmaBox_up167 (double x) const |
| double | getIntegrand_dsigmaBox_up172 (double x) const |
| double | getIntegrand_dsigmaBox_up183 (double x) const |
| double | getIntegrand_dsigmaBox_up189 (double x) const |
| double | getIntegrand_dsigmaBox_up192 (double x) const |
| double | getIntegrand_dsigmaBox_up196 (double x) const |
| double | getIntegrand_dsigmaBox_up200 (double x) const |
| double | getIntegrand_dsigmaBox_up202 (double x) const |
| double | getIntegrand_dsigmaBox_up205 (double x) const |
| double | getIntegrand_dsigmaBox_up207 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom130 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom133 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom136 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom161 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom167 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom172 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom183 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom189 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom192 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom196 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom200 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom202 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom205 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom207 (double x) const |
| double | getIntegrand_sigmaWithISR_charm130 (double x) const |
| double | getIntegrand_sigmaWithISR_charm133 (double x) const |
| double | getIntegrand_sigmaWithISR_charm136 (double x) const |
| double | getIntegrand_sigmaWithISR_charm161 (double x) const |
| double | getIntegrand_sigmaWithISR_charm167 (double x) const |
| double | getIntegrand_sigmaWithISR_charm172 (double x) const |
| double | getIntegrand_sigmaWithISR_charm183 (double x) const |
| double | getIntegrand_sigmaWithISR_charm189 (double x) const |
| double | getIntegrand_sigmaWithISR_charm192 (double x) const |
| double | getIntegrand_sigmaWithISR_charm196 (double x) const |
| double | getIntegrand_sigmaWithISR_charm200 (double x) const |
| double | getIntegrand_sigmaWithISR_charm202 (double x) const |
| double | getIntegrand_sigmaWithISR_charm205 (double x) const |
| double | getIntegrand_sigmaWithISR_charm207 (double x) const |
| double | getIntegrand_sigmaWithISR_down130 (double x) const |
| double | getIntegrand_sigmaWithISR_down133 (double x) const |
| double | getIntegrand_sigmaWithISR_down136 (double x) const |
| double | getIntegrand_sigmaWithISR_down161 (double x) const |
| double | getIntegrand_sigmaWithISR_down167 (double x) const |
| double | getIntegrand_sigmaWithISR_down172 (double x) const |
| double | getIntegrand_sigmaWithISR_down183 (double x) const |
| double | getIntegrand_sigmaWithISR_down189 (double x) const |
| double | getIntegrand_sigmaWithISR_down192 (double x) const |
| double | getIntegrand_sigmaWithISR_down196 (double x) const |
| double | getIntegrand_sigmaWithISR_down200 (double x) const |
| double | getIntegrand_sigmaWithISR_down202 (double x) const |
| double | getIntegrand_sigmaWithISR_down205 (double x) const |
| double | getIntegrand_sigmaWithISR_down207 (double x) const |
| double | getIntegrand_sigmaWithISR_mu130 (double x) const |
| double | getIntegrand_sigmaWithISR_mu136 (double x) const |
| double | getIntegrand_sigmaWithISR_mu161 (double x) const |
| double | getIntegrand_sigmaWithISR_mu172 (double x) const |
| double | getIntegrand_sigmaWithISR_mu183 (double x) const |
| double | getIntegrand_sigmaWithISR_mu189 (double x) const |
| double | getIntegrand_sigmaWithISR_mu192 (double x) const |
| double | getIntegrand_sigmaWithISR_mu196 (double x) const |
| double | getIntegrand_sigmaWithISR_mu200 (double x) const |
| double | getIntegrand_sigmaWithISR_mu202 (double x) const |
| double | getIntegrand_sigmaWithISR_mu205 (double x) const |
| double | getIntegrand_sigmaWithISR_mu207 (double x) const |
| double | getIntegrand_sigmaWithISR_strange130 (double x) const |
| double | getIntegrand_sigmaWithISR_strange133 (double x) const |
| double | getIntegrand_sigmaWithISR_strange136 (double x) const |
| double | getIntegrand_sigmaWithISR_strange161 (double x) const |
| double | getIntegrand_sigmaWithISR_strange167 (double x) const |
| double | getIntegrand_sigmaWithISR_strange172 (double x) const |
| double | getIntegrand_sigmaWithISR_strange183 (double x) const |
| double | getIntegrand_sigmaWithISR_strange189 (double x) const |
| double | getIntegrand_sigmaWithISR_strange192 (double x) const |
| double | getIntegrand_sigmaWithISR_strange196 (double x) const |
| double | getIntegrand_sigmaWithISR_strange200 (double x) const |
| double | getIntegrand_sigmaWithISR_strange202 (double x) const |
| double | getIntegrand_sigmaWithISR_strange205 (double x) const |
| double | getIntegrand_sigmaWithISR_strange207 (double x) const |
| double | getIntegrand_sigmaWithISR_tau130 (double x) const |
| double | getIntegrand_sigmaWithISR_tau136 (double x) const |
| double | getIntegrand_sigmaWithISR_tau161 (double x) const |
| double | getIntegrand_sigmaWithISR_tau172 (double x) const |
| double | getIntegrand_sigmaWithISR_tau183 (double x) const |
| double | getIntegrand_sigmaWithISR_tau189 (double x) const |
| double | getIntegrand_sigmaWithISR_tau192 (double x) const |
| double | getIntegrand_sigmaWithISR_tau196 (double x) const |
| double | getIntegrand_sigmaWithISR_tau200 (double x) const |
| double | getIntegrand_sigmaWithISR_tau202 (double x) const |
| double | getIntegrand_sigmaWithISR_tau205 (double x) const |
| double | getIntegrand_sigmaWithISR_tau207 (double x) const |
| double | getIntegrand_sigmaWithISR_up130 (double x) const |
| double | getIntegrand_sigmaWithISR_up133 (double x) const |
| double | getIntegrand_sigmaWithISR_up136 (double x) const |
| double | getIntegrand_sigmaWithISR_up161 (double x) const |
| double | getIntegrand_sigmaWithISR_up167 (double x) const |
| double | getIntegrand_sigmaWithISR_up172 (double x) const |
| double | getIntegrand_sigmaWithISR_up183 (double x) const |
| double | getIntegrand_sigmaWithISR_up189 (double x) const |
| double | getIntegrand_sigmaWithISR_up192 (double x) const |
| double | getIntegrand_sigmaWithISR_up196 (double x) const |
| double | getIntegrand_sigmaWithISR_up200 (double x) const |
| double | getIntegrand_sigmaWithISR_up202 (double x) const |
| double | getIntegrand_sigmaWithISR_up205 (double x) const |
| double | getIntegrand_sigmaWithISR_up207 (double x) const |
| double | Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| double | Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| double | Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const |
| double | Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const |
| double | Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) 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... | |
| double | sigma_NoISR_l (const QCD::lepton l_flavor, const double s) 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 | |
| double | MassOfNf (int nf) const |
| The Mbar mass of the heaviest quark in the theory with Nf active flavour. More... | |
Protected Attributes | |
| double | CdH_11i |
| The dimension-6 operator coefficient \((C_{DH})_{11}\) (imaginary part). More... | |
| double | CdH_11r |
| The dimension-6 operator coefficient \((C_{DH})_{11}\) (real part). More... | |
| double | CdH_12i |
| The dimension-6 operator coefficient \((C_{DH})_{12}\) (imaginary part). More... | |
| double | CdH_12r |
| The dimension-6 operator coefficient \((C_{DH})_{12}\) (real part). More... | |
| double | CdH_13i |
| The dimension-6 operator coefficient \((C_{DH})_{13}\) (imaginary part). More... | |
| double | CdH_13r |
| The dimension-6 operator coefficient \((C_{DH})_{13}\) (real part). More... | |
| double | CdH_22i |
| The dimension-6 operator coefficient \((C_{DH})_{22}\) (imaginary part). More... | |
| double | CdH_22r |
| The dimension-6 operator coefficient \((C_{DH})_{22}\) (real part). More... | |
| double | CdH_23i |
| The dimension-6 operator coefficient \((C_{DH})_{23}\) (imaginary part). More... | |
| double | CdH_23r |
| The dimension-6 operator coefficient \((C_{DH})_{23}\) (real part). More... | |
| double | CdH_33i |
| The dimension-6 operator coefficient \((C_{DH})_{33}\) (imaginary part). More... | |
| double | CdH_33r |
| The dimension-6 operator coefficient \((C_{DH})_{33}\) (real part). More... | |
| double | CDHB |
| The dimension-6 operator coefficient \(C_{DHB}\). More... | |
| double | CDHW |
| The dimension-6 operator coefficient \(C_{DHW}\). More... | |
| double | Ced |
| The dimension-6 (four-fermion) operator coefficient \(C_{ED}\). More... | |
| double | Cee |
| The dimension-6 (four-fermion) operator coefficient \(C_{EE}\). More... | |
| double | CeH_11i |
| The dimension-6 operator coefficient \((C_{EH})_{11}\) (imaginary part). More... | |
| double | CeH_11r |
| The dimension-6 operator coefficient \((C_{EH})_{11}\) (real part). More... | |
| double | CeH_12i |
| The dimension-6 operator coefficient \((C_{EH})_{12}\) (imaginary part). More... | |
| double | CeH_12r |
| The dimension-6 operator coefficient \((C_{EH})_{12}\) (real part). More... | |
| double | CeH_13i |
| The dimension-6 operator coefficient \((C_{EH})_{13}\) (imaginary part). More... | |
| double | CeH_13r |
| The dimension-6 operator coefficient \((C_{EH})_{13}\) (real part). More... | |
| double | CeH_22i |
| The dimension-6 operator coefficient \((C_{EH})_{22}\) (imaginary part). More... | |
| double | CeH_22r |
| The dimension-6 operator coefficient \((C_{EH})_{22}\) (real part). More... | |
| double | CeH_23i |
| The dimension-6 operator coefficient \((C_{EH})_{23}\) (imaginary part). More... | |
| double | CeH_23r |
| The dimension-6 operator coefficient \((C_{EH})_{23}\) (real part). More... | |
| double | CeH_33i |
| The dimension-6 operator coefficient \((C_{EH})_{33}\) (imaginary part). More... | |
| double | CeH_33r |
| The dimension-6 operator coefficient \((C_{EH})_{33}\) (real part). More... | |
| double | Ceu |
| The dimension-6 (four-fermion) operator coefficient \(C_{EU}\). More... | |
| double | CG |
| The dimension-6 operator coefficient \(C_{G}\). More... | |
| double | CH |
| The dimension-6 operator coefficient \(C_{H}\). More... | |
| double | CHB |
| The dimension-6 operator coefficient \(C_{HB}\). More... | |
| double | CHbox |
| The dimension-6 operator coefficient \(C_{H\Box}\). More... | |
| double | CHd_11 |
| The dimension-6 operator coefficient \((C_{HD})_{11}\). More... | |
| double | CHd_12i |
| The dimension-6 operator coefficient \((C_{HD})_{12}\) (imaginary part). More... | |
| double | CHd_12r |
| The dimension-6 operator coefficient \((C_{HD})_{12}\) (real part). More... | |
| double | CHd_13i |
| The dimension-6 operator coefficient \((C_{HD})_{13}\) (imaginary part). More... | |
| double | CHd_13r |
| The dimension-6 operator coefficient \((C_{HD})_{13}\) (real part). More... | |
| double | CHd_22 |
| The dimension-6 operator coefficient \((C_{HD})_{22}\). More... | |
| double | CHd_23i |
| The dimension-6 operator coefficient \((C_{HD})_{23}\) (imaginary part). More... | |
| double | CHd_23r |
| The dimension-6 operator coefficient \((C_{HD})_{23}\) (real part). More... | |
| double | CHd_33 |
| The dimension-6 operator coefficient \((C_{HD})_{33}\). More... | |
| double | CHe_11 |
| The dimension-6 operator coefficient \((C_{HE})_{11}\). More... | |
| double | CHe_12i |
| The dimension-6 operator coefficient \((C_{HE})_{12}\) (imaginary part). More... | |
| double | CHe_12r |
| The dimension-6 operator coefficient \((C_{HE})_{12}\) (real part). More... | |
| double | CHe_13i |
| The dimension-6 operator coefficient \((C_{HE})_{13}\) (imaginary part). More... | |
| double | CHe_13r |
| The dimension-6 operator coefficient \((C_{HE})_{13}\) (real part). More... | |
| double | CHe_22 |
| The dimension-6 operator coefficient \((C_{HE})_{22}\). More... | |
| double | CHe_23i |
| The dimension-6 operator coefficient \((C_{HE})_{23}\) (imaginary part). More... | |
| double | CHe_23r |
| The dimension-6 operator coefficient \((C_{HE})_{23}\) (real part). More... | |
| double | CHe_33 |
| The dimension-6 operator coefficient \((C_{HE})_{33}\). More... | |
| double | CHG |
| The dimension-6 operator coefficient \(C_{HG}\). More... | |
| double | CHL1_11 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\). More... | |
| double | CHL1_12i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part). More... | |
| double | CHL1_12r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part). More... | |
| double | CHL1_13i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part). More... | |
| double | CHL1_13r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part). More... | |
| double | CHL1_22 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\). More... | |
| double | CHL1_23i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part). More... | |
| double | CHL1_23r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part). More... | |
| double | CHL1_33 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\). More... | |
| double | CHL3_11 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\). More... | |
| double | CHL3_12i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More... | |
| double | CHL3_12r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More... | |
| double | CHL3_13i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More... | |
| double | CHL3_13r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More... | |
| double | CHL3_22 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\). More... | |
| double | CHL3_23i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More... | |
| double | CHL3_23r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More... | |
| double | CHL3_33 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\). More... | |
| double | CHQ1_11 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\). More... | |
| double | CHQ1_12i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part). More... | |
| double | CHQ1_12r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part). More... | |
| double | CHQ1_13i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part). More... | |
| double | CHQ1_13r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part). More... | |
| double | CHQ1_22 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\). More... | |
| double | CHQ1_23i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part). More... | |
| double | CHQ1_23r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part). More... | |
| double | CHQ1_33 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\). More... | |
| double | CHQ3_11 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\). More... | |
| double | CHQ3_12i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part). More... | |
| double | CHQ3_12r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part). More... | |
| double | CHQ3_13i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part). More... | |
| double | CHQ3_13r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part). More... | |
| double | CHQ3_22 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\). More... | |
| double | CHQ3_23i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part). More... | |
| double | CHQ3_23r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part). More... | |
| double | CHQ3_33 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\). More... | |
| double | CHu_11 |
| The dimension-6 operator coefficient \((C_{HU})_{11}\). More... | |
| double | CHu_12i |
| The dimension-6 operator coefficient \((C_{HU})_{12}\) (imaginary part). More... | |
| double | CHu_12r |
| The dimension-6 operator coefficient \((C_{HU})_{12}\) (real part). More... | |
| double | CHu_13i |
| The dimension-6 operator coefficient \((C_{HU})_{13}\) (imaginary part). More... | |
| double | CHu_13r |
| The dimension-6 operator coefficient \((C_{HU})_{13}\) (real part). More... | |
| double | CHu_22 |
| The dimension-6 operator coefficient \((C_{HU})_{22}\). More... | |
| double | CHu_23i |
| The dimension-6 operator coefficient \((C_{HU})_{23}\) (imaginary part). More... | |
| double | CHu_23r |
| The dimension-6 operator coefficient \((C_{HU})_{23}\) (real part). More... | |
| double | CHu_33 |
| The dimension-6 operator coefficient \((C_{HU})_{33}\). More... | |
| double | CHud_11i |
| The dimension-6 operator coefficient \((C_{HUD})_{11}\) (imaginary part). More... | |
| double | CHud_11r |
| The dimension-6 operator coefficient \((C_{HUD})_{11}\) (real part). More... | |
| double | CHud_12i |
| The dimension-6 operator coefficient \((C_{HUD})_{12}\) (imaginary part). More... | |
| double | CHud_12r |
| The dimension-6 operator coefficient \((C_{HUD})_{12}\) (real part). More... | |
| double | CHud_13i |
| The dimension-6 operator coefficient \((C_{HUD})_{13}\) (imaginary part). More... | |
| double | CHud_13r |
| The dimension-6 operator coefficient \((C_{HUD})_{13}\) (real part). More... | |
| double | CHud_22i |
| The dimension-6 operator coefficient \((C_{HUD})_{22}\) (imaginary part). More... | |
| double | CHud_22r |
| The dimension-6 operator coefficient \((C_{HUD})_{22}\) (real part). More... | |
| double | CHud_23i |
| The dimension-6 operator coefficient \((C_{HUD})_{23}\) (imaginary part). More... | |
| double | CHud_23r |
| The dimension-6 operator coefficient \((C_{HUD})_{23}\) (real part). More... | |
| double | CHud_33i |
| The dimension-6 operator coefficient \((C_{HUD})_{33}\) (imaginary part). More... | |
| double | CHud_33r |
| The dimension-6 operator coefficient \((C_{HUD})_{33}\) (real part). More... | |
| double | CHW |
| The dimension-6 operator coefficient \(C_{HW}\). More... | |
| double | CHWHB_gaga |
| The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\). More... | |
| double | CHWHB_gagaorth |
| The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\). More... | |
| double | CLd |
| The dimension-6 (four-fermion) operator coefficient \(C_{LD}\). More... | |
| double | CLe |
| The dimension-6 (four-fermion) operator coefficient \(C_{LE}\). More... | |
| double | CLL_1221 |
| The dimension-6 operator coefficient \((C_{LL})_{1221}\). More... | |
| double | CLL_2112 |
| The dimension-6 operator coefficient \((C_{LL})_{2112}\). More... | |
| double | CLQ1 |
| The dimension-6 (four-fermion) operator coefficient \(C_{LQ}^{(1)}\). More... | |
| double | CLQ3 |
| The dimension-6 (four-fermion) operator coefficient \(C_{LQ}^{(3)}\). More... | |
| double | CLu |
| The dimension-6 (four-fermion) operator coefficient \(C_{LU}\). More... | |
| double | CQe |
| The dimension-6 (four-fermion) operator coefficient \(C_{QE}\). More... | |
| double | CuB_11i |
| The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part). More... | |
| double | CuB_11r |
| The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part). More... | |
| double | CuB_12i |
| The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part). More... | |
| double | CuB_12r |
| The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part). More... | |
| double | CuB_13i |
| The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part). More... | |
| double | CuB_13r |
| The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part). More... | |
| double | CuB_22i |
| The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part). More... | |
| double | CuB_22r |
| The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part). More... | |
| double | CuB_23i |
| The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part). More... | |
| double | CuB_23r |
| The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part). More... | |
| double | CuB_33i |
| The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part). More... | |
| double | CuB_33r |
| The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part). More... | |
| double | CuG_11i |
| The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part). More... | |
| double | CuG_11r |
| The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part). More... | |
| double | CuG_12i |
| The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part). More... | |
| double | CuG_12r |
| The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part). More... | |
| double | CuG_13i |
| The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part). More... | |
| double | CuG_13r |
| The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part). More... | |
| double | CuG_22i |
| The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part). More... | |
| double | CuG_22r |
| The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part). More... | |
| double | CuG_23i |
| The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part). More... | |
| double | CuG_23r |
| The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part). More... | |
| double | CuG_33i |
| The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part). More... | |
| double | CuG_33r |
| The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part). More... | |
| double | CuH_11i |
| The dimension-6 operator coefficient \((C_{UH})_{11}\) (imaginary part). More... | |
| double | CuH_11r |
| The dimension-6 operator coefficient \((C_{UH})_{11}\) (real part). More... | |
| double | CuH_12i |
| The dimension-6 operator coefficient \((C_{UH})_{12}\) (imaginary part). More... | |
| double | CuH_12r |
| The dimension-6 operator coefficient \((C_{UH})_{12}\) (real part). More... | |
| double | CuH_13i |
| The dimension-6 operator coefficient \((C_{UH})_{13}\) (imaginary part). More... | |
| double | CuH_13r |
| The dimension-6 operator coefficient \((C_{UH})_{13}\) (real part). More... | |
| double | CuH_22i |
| The dimension-6 operator coefficient \((C_{UH})_{22}\) (imaginary part). More... | |
| double | CuH_22r |
| The dimension-6 operator coefficient \((C_{UH})_{22}\) (real part). More... | |
| double | CuH_23i |
| The dimension-6 operator coefficient \((C_{UH})_{23}\) (imaginary part). More... | |
| double | CuH_23r |
| The dimension-6 operator coefficient \((C_{UH})_{23}\) (real part). More... | |
| double | CuH_33i |
| The dimension-6 operator coefficient \((C_{UH})_{33}\) (imaginary part). More... | |
| double | CuH_33r |
| The dimension-6 operator coefficient \((C_{UH})_{33}\) (real part). More... | |
| double | CuW_11i |
| The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part). More... | |
| double | CuW_11r |
| The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part). More... | |
| double | CuW_12i |
| The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part). More... | |
| double | CuW_12r |
| The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part). More... | |
| double | CuW_13i |
| The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part). More... | |
| double | CuW_13r |
| The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part). More... | |
| double | CuW_22i |
| The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part). More... | |
| double | CuW_22r |
| The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part). More... | |
| double | CuW_23i |
| The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part). More... | |
| double | CuW_23r |
| The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part). More... | |
| double | CuW_33i |
| The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part). More... | |
| double | CuW_33r |
| The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part). More... | |
| double | CW |
| The dimension-6 operator coefficient \(C_{W}\). More... | |
| double | cW2_tree |
| The sqaure of the tree level values for the cosine of the weak angle. More... | |
| double | cW_tree |
| The tree level values for the cosine of the weak angle. More... | |
| double | delta_AA |
| Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More... | |
| double | delta_AZ |
| Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More... | |
| double | delta_h |
| Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition. More... | |
| double | delta_ZZ |
| Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition. More... | |
| double | ettH2_Hgg |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to ttH production at Tevatron (1.96 TeV). More... | |
| double | ettH2_Htt |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Htt}\) to ttH production at Tevatron (1.96 TeV). More... | |
| double | ettH78_Hgg |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to ttH production at the LHC (7 & 8 TeV). More... | |
| double | ettH78_Htt |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Htt}\) to ttH production at the LHC (7 & 8 TeV). More... | |
| double | eVBF2_HAA |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HAA}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_Hgg |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HWud |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HWW1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HWW2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HWW3 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HZA1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HZA2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HZdL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HZdR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HZuL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HZuR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HZZ1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HZZ2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_HZZ3 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_Wud |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_ZdL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_ZdR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_ZuL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF2_ZuR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF78_HAA |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HAA}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_Hgg |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HWud |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HWW1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HWW2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HWW3 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HZA1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HZA2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HZdL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HZdR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HZuL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HZuR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HZZ1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HZZ2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_HZZ3 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_Wud |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_ZdL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_ZdR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_ZuL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eVBF78_ZuR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to VBF production at the LHC (7 & 8 TeV). More... | |
| double | eWH2_HWud |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH2_HWW1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH2_HWW2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH2_HWW3 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH2_Wud |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH78_HWud |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eWH78_HWW1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eWH78_HWW2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eWH78_HWW3 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eWH78_Wud |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eZH2_HZA1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_HZA2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_HZdL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_HZdR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_HZuL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_HZuR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_HZZ1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_HZZ2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_HZZ3 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_ZdL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_ZdR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_ZuL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH2_ZuR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH78_HZA1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_HZA2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_HZdL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_HZdR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_HZuL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_HZuR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_HZZ1 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_HZZ2 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_HZZ3 |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_ZdL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_ZdR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_ZuL |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | eZH78_ZuR |
| Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to ZH production at the LHC (7 & 8 TeV). More... | |
| double | Lambda_NP |
| The new physics scale [GeV]. More... | |
| double | LambdaNP2 |
| The square of the new physics scale [GeV \(^2\)]. More... | |
| double | MwInput |
| The input value for the \(W\)-boson mass if FlagMwInput is true. More... | |
| double | sW2_tree |
| The sqaure of the tree level values for the sine of the weak angle. More... | |
| double | sW_tree |
| The tree level values for the sine of the weak angle. More... | |
| double | v2_over_LambdaNP2 |
| The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\). 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 | alpha21 |
| double | alpha31 |
| double | AlsMz |
| The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More... | |
| bool | bSigmaForAFB |
| bool | bSigmaForR |
| 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 | 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 | 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... | |
| 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 | 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 |
| 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... | |
| 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 |
| 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 |
| A boolean set to false if update is successful. More... | |
Private Attributes | |
| const bool | FlagLeptonUniversal |
| An internal boolean flag that is true if assuming lepton flavour universality. More... | |
| bool | FlagMwInput |
| A boolean flag that is true if the W mass is taken as an input parameter. (Warning: The W width is not implemented in this case.) More... | |
| bool | FlagQuadraticTerms |
| A boolean flag that is true if the quadratic terms in cross sections and widths are switched on. More... | |
| const bool | FlagQuarkUniversal |
| An internal boolean flag that is true if assuming quark flavour universality. More... | |
| bool | FlagRotateCHWCHB |
| A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB. 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, B_D, B_P, B_S, B_C, PHI, K_star, K_star_P, 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... | |
| NPEffectiveGIMRprime::NPEffectiveGIMRprime | ( | 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 157 of file NPEffectiveGIMRprime.cpp.
| gslpp::complex NPEffectiveGIMRprime::AH_f | ( | const double | tau | ) | const |
Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.
\(A^H_f(\tau)=2\tau [1+(1-\tau)f(\tau)]\)
| [in] |
Definition at line 1722 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2731 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2711 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2651 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2571 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2671 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2691 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2591 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2631 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2611 of file NPEffectiveGIMRprime.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 1406 of file NPEffectiveGIMRprime.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 1354 of file NPEffectiveGIMRprime.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 1328 of file NPEffectiveGIMRprime.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 1380 of file NPEffectiveGIMRprime.cpp.
|
virtual |
A method to check if all the mandatory parameters for NPEffectiveGIMRprime 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 1163 of file NPEffectiveGIMRprime.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F.
| [in] | F | a lepton or quark |
Definition at line 1251 of file NPEffectiveGIMRprime.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F.
| [in] | F | a lepton or quark |
Definition at line 1269 of file NPEffectiveGIMRprime.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 1287 of file NPEffectiveGIMRprime.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HUD}\) corresponding to particle f.
| [in] | u | a quark |
Definition at line 1313 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2751 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 1557 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 1597 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 1580 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 1562 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 1602 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 1585 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).
Reimplemented from NPbase.
Definition at line 1567 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).
Reimplemented from NPbase.
Definition at line 1590 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltag3G | ( | ) | const |
The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\).
Definition at line 1700 of file NPEffectiveGIMRprime.cpp.
| gslpp::complex NPEffectiveGIMRprime::deltaG_Aff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 1693 of file NPEffectiveGIMRprime.cpp.
| gslpp::complex NPEffectiveGIMRprime::deltaG_Gff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 1679 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 1607 of file NPEffectiveGIMRprime.cpp.
| gslpp::complex NPEffectiveGIMRprime::deltaG_hAff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 1672 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 1612 of file NPEffectiveGIMRprime.cpp.
| gslpp::complex NPEffectiveGIMRprime::deltaG_hGff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 1658 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).
Reimplemented from NPbase.
Definition at line 1552 of file NPEffectiveGIMRprime.cpp.
| gslpp::complex NPEffectiveGIMRprime::deltaG_hZff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 1665 of file NPEffectiveGIMRprime.cpp.
| gslpp::complex NPEffectiveGIMRprime::deltaG_Zff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 1686 of file NPEffectiveGIMRprime.cpp.
|
virtual |
New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 1483 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHbbRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 3078 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHbbRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 3084 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHccRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 3050 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHccRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 3055 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHgagaRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2950 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHgagaRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 2961 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHggRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.
Definition at line 2806 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHggRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 2814 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHmumuRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2990 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHmumuRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 2996 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHtautauRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 3020 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHtautauRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 3026 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHWWRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2841 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHWWRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 2850 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHZgaRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2910 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHZgaRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 2922 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHZZRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2875 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGammaHZZRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 2884 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.
Definition at line 2764 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.
Definition at line 2777 of file NPEffectiveGIMRprime.cpp.
|
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 experimental value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM.
Reimplemented from NPbase.
Definition at line 1435 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGL_f | ( | const Particle | p | ) | const |
New physics contribution to the neutral-current left-handed coupling \(g_L^f\).
| [in] | f | a lepton or quark |
Definition at line 1488 of file NPEffectiveGIMRprime.cpp.
|
virtual |
New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 1526 of file NPEffectiveGIMRprime.cpp.
| gslpp::complex NPEffectiveGIMRprime::deltaGL_Wffh | ( | const Particle | pbar, |
| const Particle | p | ||
| ) | const |
The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Definition at line 1626 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGL_Zffh | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | p | a lepton or quark |
Definition at line 1644 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGR_f | ( | const Particle | p | ) | const |
New physics contribution to the neutral-current right-handed coupling \(g_R^f\).
| [in] | f | a lepton or quark |
Definition at line 1507 of file NPEffectiveGIMRprime.cpp.
|
virtual |
New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 1543 of file NPEffectiveGIMRprime.cpp.
| gslpp::complex NPEffectiveGIMRprime::deltaGR_Wffh | ( | const Particle | pbar, |
| const Particle | p | ||
| ) | const |
The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Definition at line 1635 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::deltaGR_Zffh | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | p | a lepton or quark |
Definition at line 1652 of file NPEffectiveGIMRprime.cpp.
|
virtual |
New physics contribution to the neutral-current vector coupling \(g_V^f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 1478 of file NPEffectiveGIMRprime.cpp.
| gslpp::complex NPEffectiveGIMRprime::f_triangle | ( | const double | tau | ) | const |
Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.
| [in] |
Definition at line 1710 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::GammaHbbRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model.
Definition at line 3063 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::GammaHccRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model.
Definition at line 3034 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::GammaHgagaRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model.
Definition at line 2934 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::GammaHggRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model.
Definition at line 2790 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::GammaHmumuRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model.
Definition at line 2974 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::GammaHtautauRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model.
Definition at line 3004 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::GammaHWWRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model.
Definition at line 2825 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::GammaHZgaRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model.
Definition at line 2894 of file NPEffectiveGIMRprime.cpp.
| double NPEffectiveGIMRprime::GammaHZZRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model.
Definition at line 2859 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The total width of the \(W\) boson, \(\Gamma_W\).
Reimplemented from NPbase.
Definition at line 1464 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 2506 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1956 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 2304 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1727 of file NPEffectiveGIMRprime.cpp.
|
virtual |
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.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 2492 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 2437 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1763 of file NPEffectiveGIMRprime.cpp.
|
virtual |
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.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 2422 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 2409 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 2087 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 2162 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The mass of the \(W\) boson, \(M_W\).
Reimplemented from NPbase.
Definition at line 1455 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The oblique parameter \(S\).
Reimplemented from NPbase.
Definition at line 1440 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The oblique parameter \(T\).
Reimplemented from NPbase.
Definition at line 1445 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The oblique parameter \(U\).
Reimplemented from NPbase.
Definition at line 1450 of file NPEffectiveGIMRprime.cpp.
|
virtual |
The post-update method for NPEffectiveGIMRprime.
This method runs all the procedures that are need to be executed after the model is successfully updated.
Reimplemented from NPbase.
Definition at line 455 of file NPEffectiveGIMRprime.cpp.
|
virtual |
A method to set a flag of NPEffectiveGIMRprime.
| [in] | name | name of a model flag |
| [in] | value | the boolean to be assigned to the flag specified by name |
Reimplemented from StandardModel.
Definition at line 1229 of file NPEffectiveGIMRprime.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 485 of file NPEffectiveGIMRprime.cpp.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{11}\) (imaginary part).
Definition at line 1405 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{11}\) (real part).
Definition at line 1399 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{12}\) (imaginary part).
Definition at line 1406 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{12}\) (real part).
Definition at line 1400 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{13}\) (imaginary part).
Definition at line 1407 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{13}\) (real part).
Definition at line 1401 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{22}\) (imaginary part).
Definition at line 1408 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{22}\) (real part).
Definition at line 1402 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{23}\) (imaginary part).
Definition at line 1409 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{23}\) (real part).
Definition at line 1403 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{33}\) (imaginary part).
Definition at line 1410 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{DH})_{33}\) (real part).
Definition at line 1404 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \(C_{DHB}\).
Definition at line 1296 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \(C_{DHW}\).
Definition at line 1297 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 (four-fermion) operator coefficient \(C_{ED}\).
Definition at line 1453 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 (four-fermion) operator coefficient \(C_{EE}\).
Definition at line 1451 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{11}\) (imaginary part).
Definition at line 1381 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{11}\) (real part).
Definition at line 1375 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{12}\) (imaginary part).
Definition at line 1382 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{12}\) (real part).
Definition at line 1376 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{13}\) (imaginary part).
Definition at line 1383 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{13}\) (real part).
Definition at line 1377 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{22}\) (imaginary part).
Definition at line 1384 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{22}\) (real part).
Definition at line 1378 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{23}\) (imaginary part).
Definition at line 1385 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{23}\) (real part).
Definition at line 1379 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{33}\) (imaginary part).
Definition at line 1386 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{EH})_{33}\) (real part).
Definition at line 1380 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 (four-fermion) operator coefficient \(C_{EU}\).
Definition at line 1452 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \(C_{G}\).
Definition at line 1289 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \(C_{H}\).
Definition at line 1299 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \(C_{HB}\).
Definition at line 1293 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \(C_{H\Box}\).
Definition at line 1298 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HD})_{11}\).
Definition at line 1354 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HD})_{12}\) (imaginary part).
Definition at line 1360 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HD})_{12}\) (real part).
Definition at line 1355 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HD})_{13}\) (imaginary part).
Definition at line 1361 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HD})_{13}\) (real part).
Definition at line 1356 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HD})_{22}\).
Definition at line 1357 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HD})_{23}\) (imaginary part).
Definition at line 1362 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HD})_{23}\) (real part).
Definition at line 1358 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HD})_{33}\).
Definition at line 1359 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HE})_{11}\).
Definition at line 1318 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HE})_{12}\) (imaginary part).
Definition at line 1324 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HE})_{12}\) (real part).
Definition at line 1319 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HE})_{13}\) (imaginary part).
Definition at line 1325 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HE})_{13}\) (real part).
Definition at line 1320 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HE})_{22}\).
Definition at line 1321 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HE})_{23}\) (imaginary part).
Definition at line 1326 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HE})_{23}\) (real part).
Definition at line 1322 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HE})_{33}\).
Definition at line 1323 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \(C_{HG}\).
Definition at line 1291 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\).
Definition at line 1300 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part).
Definition at line 1306 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part).
Definition at line 1301 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part).
Definition at line 1307 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part).
Definition at line 1302 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\).
Definition at line 1303 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part).
Definition at line 1308 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part).
Definition at line 1304 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\).
Definition at line 1305 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\).
Definition at line 1309 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).
Definition at line 1315 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).
Definition at line 1310 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).
Definition at line 1316 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).
Definition at line 1311 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\).
Definition at line 1312 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).
Definition at line 1317 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).
Definition at line 1313 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\).
Definition at line 1314 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\).
Definition at line 1327 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part).
Definition at line 1333 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part).
Definition at line 1328 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part).
Definition at line 1334 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part).
Definition at line 1329 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\).
Definition at line 1330 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part).
Definition at line 1335 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part).
Definition at line 1331 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\).
Definition at line 1332 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\).
Definition at line 1336 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part).
Definition at line 1342 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part).
Definition at line 1337 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part).
Definition at line 1343 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part).
Definition at line 1338 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\).
Definition at line 1339 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part).
Definition at line 1344 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part).
Definition at line 1340 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\).
Definition at line 1341 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HU})_{11}\).
Definition at line 1345 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HU})_{12}\) (imaginary part).
Definition at line 1351 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HU})_{12}\) (real part).
Definition at line 1346 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HU})_{13}\) (imaginary part).
Definition at line 1352 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HU})_{13}\) (real part).
Definition at line 1347 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HU})_{22}\).
Definition at line 1348 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HU})_{23}\) (imaginary part).
Definition at line 1353 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HU})_{23}\) (real part).
Definition at line 1349 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HU})_{33}\).
Definition at line 1350 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{11}\) (imaginary part).
Definition at line 1369 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{11}\) (real part).
Definition at line 1363 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{12}\) (imaginary part).
Definition at line 1370 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{12}\) (real part).
Definition at line 1364 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{13}\) (imaginary part).
Definition at line 1371 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{13}\) (real part).
Definition at line 1365 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{22}\) (imaginary part).
Definition at line 1372 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{22}\) (real part).
Definition at line 1366 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{23}\) (imaginary part).
Definition at line 1373 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{23}\) (real part).
Definition at line 1367 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{33}\) (imaginary part).
Definition at line 1374 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{HUD})_{33}\) (real part).
Definition at line 1368 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \(C_{HW}\).
Definition at line 1292 of file NPEffectiveGIMRprime.h.
|
protected |
The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\).
Definition at line 1294 of file NPEffectiveGIMRprime.h.
|
protected |
The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\).
Definition at line 1295 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 (four-fermion) operator coefficient \(C_{LD}\).
Definition at line 1456 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 (four-fermion) operator coefficient \(C_{LE}\).
Definition at line 1454 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{LL})_{1221}\).
Definition at line 1447 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{LL})_{2112}\).
Definition at line 1448 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 (four-fermion) operator coefficient \(C_{LQ}^{(1)}\).
Definition at line 1449 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 (four-fermion) operator coefficient \(C_{LQ}^{(3)}\).
Definition at line 1450 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 (four-fermion) operator coefficient \(C_{LU}\).
Definition at line 1455 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 (four-fermion) operator coefficient \(C_{QE}\).
Definition at line 1457 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part).
Definition at line 1441 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part).
Definition at line 1435 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part).
Definition at line 1442 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part).
Definition at line 1436 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part).
Definition at line 1443 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part).
Definition at line 1437 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part).
Definition at line 1444 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part).
Definition at line 1438 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part).
Definition at line 1445 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part).
Definition at line 1439 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part).
Definition at line 1446 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part).
Definition at line 1440 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part).
Definition at line 1417 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part).
Definition at line 1411 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part).
Definition at line 1418 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part).
Definition at line 1412 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part).
Definition at line 1419 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part).
Definition at line 1413 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part).
Definition at line 1420 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part).
Definition at line 1414 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part).
Definition at line 1421 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part).
Definition at line 1415 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part).
Definition at line 1422 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part).
Definition at line 1416 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{11}\) (imaginary part).
Definition at line 1393 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{11}\) (real part).
Definition at line 1387 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{12}\) (imaginary part).
Definition at line 1394 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{12}\) (real part).
Definition at line 1388 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{13}\) (imaginary part).
Definition at line 1395 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{13}\) (real part).
Definition at line 1389 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{22}\) (imaginary part).
Definition at line 1396 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{22}\) (real part).
Definition at line 1390 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{23}\) (imaginary part).
Definition at line 1397 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{23}\) (real part).
Definition at line 1391 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{33}\) (imaginary part).
Definition at line 1398 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{UH})_{33}\) (real part).
Definition at line 1392 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part).
Definition at line 1429 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part).
Definition at line 1423 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part).
Definition at line 1430 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part).
Definition at line 1424 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part).
Definition at line 1431 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part).
Definition at line 1425 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part).
Definition at line 1432 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part).
Definition at line 1426 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part).
Definition at line 1433 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part).
Definition at line 1427 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part).
Definition at line 1434 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part).
Definition at line 1428 of file NPEffectiveGIMRprime.h.
|
protected |
The dimension-6 operator coefficient \(C_{W}\).
Definition at line 1290 of file NPEffectiveGIMRprime.h.
|
protected |
The sqaure of the tree level values for the cosine of the weak angle.
Definition at line 1550 of file NPEffectiveGIMRprime.h.
|
protected |
The tree level values for the cosine of the weak angle.
Definition at line 1548 of file NPEffectiveGIMRprime.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.
Definition at line 1553 of file NPEffectiveGIMRprime.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.
Definition at line 1554 of file NPEffectiveGIMRprime.h.
|
protected |
Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition.
Definition at line 1555 of file NPEffectiveGIMRprime.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition.
Definition at line 1552 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to ttH production at Tevatron (1.96 TeV).
Definition at line 1540 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Htt}\) to ttH production at Tevatron (1.96 TeV).
Definition at line 1539 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to ttH production at the LHC (7 & 8 TeV).
Definition at line 1542 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Htt}\) to ttH production at the LHC (7 & 8 TeV).
Definition at line 1541 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HAA}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1465 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1469 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1474 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1466 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1467 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1468 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1463 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1464 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1472 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1473 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1470 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1471 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1460 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1461 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1462 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1479 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1477 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1478 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1475 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 1476 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HAA}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1485 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1489 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1494 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1486 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1487 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1488 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1483 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1484 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1492 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1493 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1490 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1491 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1480 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1481 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1482 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1499 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1497 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1498 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1495 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to VBF production at the LHC (7 & 8 TeV).
Definition at line 1496 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to WH production at Tevatron (1.96 TeV).
Definition at line 1504 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to WH production at Tevatron (1.96 TeV).
Definition at line 1501 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to WH production at Tevatron (1.96 TeV).
Definition at line 1502 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to WH production at Tevatron (1.96 TeV).
Definition at line 1503 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to WH production at Tevatron (1.96 TeV).
Definition at line 1505 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 1509 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 1506 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 1507 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 1508 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 1510 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1515 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1516 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1519 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1520 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1517 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1518 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1512 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1513 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1514 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1523 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1524 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1521 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 1522 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1528 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1529 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1532 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1533 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1530 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1531 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1525 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1526 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1527 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1536 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1537 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1534 of file NPEffectiveGIMRprime.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to ZH production at the LHC (7 & 8 TeV).
Definition at line 1535 of file NPEffectiveGIMRprime.h.
|
private |
An internal boolean flag that is true if assuming lepton flavour universality.
Definition at line 1625 of file NPEffectiveGIMRprime.h.
|
private |
A boolean flag that is true if the W mass is taken as an input parameter. (Warning: The W width is not implemented in this case.)
Definition at line 1617 of file NPEffectiveGIMRprime.h.
|
private |
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.
Definition at line 1618 of file NPEffectiveGIMRprime.h.
|
private |
An internal boolean flag that is true if assuming quark flavour universality.
Definition at line 1631 of file NPEffectiveGIMRprime.h.
|
private |
A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB.
Definition at line 1619 of file NPEffectiveGIMRprime.h.
|
protected |
The new physics scale [GeV].
Definition at line 1458 of file NPEffectiveGIMRprime.h.
|
protected |
The square of the new physics scale [GeV \(^2\)].
Definition at line 1546 of file NPEffectiveGIMRprime.h.
|
protected |
The input value for the \(W\)-boson mass if FlagMwInput is true.
Definition at line 1544 of file NPEffectiveGIMRprime.h.
|
static |
The number of the model parameters in NPEffectiveGIMRprime.
　
Definition at line 621 of file NPEffectiveGIMRprime.h.
|
static |
The number of the model parameters in NPEffectiveGIMRprime with lepton and quark flavour universalities.
　
Definition at line 639 of file NPEffectiveGIMRprime.h.
|
static |
A string array containing the labels of the model parameters in NPEffectiveGIMRprime if the model flag FlagRotateCHWCHB=false.
Definition at line 627 of file NPEffectiveGIMRprime.h.
|
static |
A string array containing the labels of the model parameters in NPEffectiveGIMRprime with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false.
Definition at line 646 of file NPEffectiveGIMRprime.h.
|
static |
A string array containing the labels of the model parameters in NPEffectiveGIMRprime if the model flag FlagRotateCHWCHB=true.
Definition at line 633 of file NPEffectiveGIMRprime.h.
|
static |
A string array containing the labels of the model parameters in NPEffectiveGIMRprime with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true.
Definition at line 653 of file NPEffectiveGIMRprime.h.
|
protected |
The sqaure of the tree level values for the sine of the weak angle.
Definition at line 1551 of file NPEffectiveGIMRprime.h.
|
protected |
The tree level values for the sine of the weak angle.
Definition at line 1549 of file NPEffectiveGIMRprime.h.
|
protected |
The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\).
Definition at line 1547 of file NPEffectiveGIMRprime.h.
1.8.16 