A module for general Two-Higgs-Doublet models (without the assumption of a \(Z_2\) symmetry). More...
Classes | |
| class | cosalpha1_GTHDM |
| cosalpha1_GTHDM More... | |
| class | DeltaQ_GTHDM |
| DeltaQ_GTHDM. More... | |
| class | DeltaT |
| An observable class for the THDM contribution to the electroweak Peskin-Takeuchi pseudo-observable \(T\). More... | |
| class | DeltaU |
| An observable class for the GeneralTHDM contribution to the electroweak Peskin-Takeuchi pseudo-observable \(U\). More... | |
| class | etaD1atQGTHDM |
| etaD1atQGTHDM. More... | |
| class | etaD2atQGTHDM |
| etaD2atQGTHDM. More... | |
| class | etaL1atQGTHDM |
| etaL1atQGTHDM. More... | |
| class | etaL2atQGTHDM |
| etaL2atQGTHDM. More... | |
| class | etaU1atQGTHDM |
| etaU1atQGTHDM. More... | |
| class | etaU2atQGTHDM |
| etaU2atQGTHDM. More... | |
| class | g1atQGTHDM |
| g1atQGTHDM. More... | |
| class | g2atQGTHDM |
| g2atQGTHDM. More... | |
| class | g3atQGTHDM |
| g3atQGTHDM. More... | |
| class | GeneralTHDM |
| A class for general Two-Higgs-Doublet models. More... | |
| class | GeneralTHDMEWPO |
| class | GeneralTHDMgminus2_mu |
| class | GeneralTHDMHeavyHiggs |
| Base class for direct heavy Higgs search observables. More... | |
| class | GeneralTHDMMatching |
| class | GeneralTHDMRunner |
| An RGE running algorithm for the GeneralTHDM parameters. More... | |
| class | GeneralTHDMSTU |
| An observable class for the electroweak Peskin-Takeuchi pseudo-observables. More... | |
| class | GTHDMDeltaS |
| An observable class for the THDM contribution to the electroweak Peskin-Takeuchi pseudo-observable \(S\). More... | |
| class | Hobs_bb_phi2_bb_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to b\bar b\). More... | |
| class | Hobs_bb_phi2_bb_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(b\bar b \to \phi_{2}\to b\bar b\). More... | |
| class | Hobs_bb_phi2_phi1Z_bbZ_1_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_bb_phi2_phi1Z_bbZ_2_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_bb_phi2_phi1Z_bbZ_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_bb_phi2_phi3Z_bbZ_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio. More... | |
| class | Hobs_bb_phi2_tautau_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(b\bar b\to \phi_{2}\to \tau \tau\). More... | |
| class | Hobs_bb_phi2_tautau_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(b\bar b\to \phi_{2}\to \tau\tau\). More... | |
| class | Hobs_bb_phi2_tautau_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(b\bar b\to \phi_{2}\to \tau \tau\). More... | |
| class | Hobs_bb_phi2_tautau_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(b\bar b\to \phi_{2}\to \tau\tau\). More... | |
| class | Hobs_bb_phi2_tt_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(b\bar b \to \phi_{2}\to t\bar t\). More... | |
| class | Hobs_bb_phi3_bb_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to b\bar b\). More... | |
| class | Hobs_bb_phi3_bb_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(b\bar b \to \phi_{3}\to b\bar b\). More... | |
| class | Hobs_bb_phi3_phi1Z_bbZ_1_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_bb_phi3_phi1Z_bbZ_2_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_bb_phi3_phi1Z_bbZ_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_bb_phi3_phi2Z_bbZ_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio. More... | |
| class | Hobs_bb_phi3_tautau_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(b\bar b\to \phi_{3}\to \tau \tau\). More... | |
| class | Hobs_bb_phi3_tautau_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(b\bar b\to \phi_{3}\to \tau\tau\). More... | |
| class | Hobs_bb_phi3_tautau_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(b\bar b\to \phi_{3}\to \tau \tau\). More... | |
| class | Hobs_bb_phi3_tautau_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(b\bar b\to \phi_{3}\to \tau\tau\). More... | |
| class | Hobs_bb_phi3_tt_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(b\bar b \to \phi_{3}\to t\bar t\). More... | |
| class | Hobs_gg_phi2_bb_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(b\bar b \to \phi_{2}\to b\bar b\). More... | |
| class | Hobs_gg_phi2_gaga_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \gamma \gamma\). More... | |
| class | Hobs_gg_phi2_gaga_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to \gamma \gamma\). More... | |
| class | Hobs_gg_phi2_phi1phi1_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg \to \phi_{2}\to \phi_{1}\phi_{1}\). More... | |
| class | Hobs_gg_phi2_phi1phi1_bbtautau_CMS8 |
| class | Hobs_gg_phi2_phi1phi1_gagaWW_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi2_phi1Z_bbll_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi2_phi1Z_bbZ_1_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi2_phi1Z_bbZ_2_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi2_phi1Z_bbZ_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi2_phi1Z_bbZ_ATLAS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi2_phi1Z_tautaull_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi2_phi1Z_tautauZ_ATLAS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi2_phi3Z_bbZ_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio. More... | |
| class | Hobs_gg_phi2_tautau_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to \tau \tau\). More... | |
| class | Hobs_gg_phi2_tautau_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to \tau\tau\). More... | |
| class | Hobs_gg_phi2_tautau_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to \tau \tau\). More... | |
| class | Hobs_gg_phi2_tautau_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to \tau\tau\). More... | |
| class | Hobs_gg_phi2_WW_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg \to \phi_{2}\to WW\). More... | |
| class | Hobs_gg_phi2_WW_enumunu_ATLAS13 |
| class | Hobs_gg_phi2_WW_lnuqq_ATLAS13 |
| class | Hobs_gg_phi2_Zga_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to Z\gamma\). More... | |
| class | Hobs_gg_phi2_Zga_llga_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to Z\gamma\). More... | |
| class | Hobs_gg_phi2_Zga_qqga_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to Z\gamma\). More... | |
| class | Hobs_gg_phi2_ZZ_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg \to \phi_{2}\to ZZ\). More... | |
| class | Hobs_gg_phi2_ZZ_llllnunu_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to ZZ\). More... | |
| class | Hobs_gg_phi2_ZZ_llnunuqq_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to ZZ\). More... | |
| class | Hobs_gg_phi3_bb_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(b\bar b \to \phi_{3}\to b\bar b\). More... | |
| class | Hobs_gg_phi3_gaga_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to \gamma \gamma\). More... | |
| class | Hobs_gg_phi3_gaga_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to \gamma \gamma\). More... | |
| class | Hobs_gg_phi3_phi1phi1_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg \to \phi_{3}\to \phi_{1}\phi_{1}\). More... | |
| class | Hobs_gg_phi3_phi1phi1_bbtautau_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio. More... | |
| class | Hobs_gg_phi3_phi1phi1_gagaWW_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi3_phi1Z_bbll_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi3_phi1Z_bbZ_1_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi3_phi1Z_bbZ_2_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi3_phi1Z_bbZ_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi3_phi1Z_bbZ_ATLAS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi3_phi1Z_tautaull_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi3_phi1Z_tautauZ_ATLAS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_gg_phi3_phi2Z_bbZ_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio. More... | |
| class | Hobs_gg_phi3_tautau_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to \tau \tau\). More... | |
| class | Hobs_gg_phi3_tautau_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to \tau\tau\). More... | |
| class | Hobs_gg_phi3_tautau_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to \tau \tau\). More... | |
| class | Hobs_gg_phi3_tautau_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to \tau\tau\). More... | |
| class | Hobs_gg_phi3_WW_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg \to \phi_{3}\to WW\). More... | |
| class | Hobs_gg_phi3_WW_enumunu_ATLAS13 |
| class | Hobs_gg_phi3_WW_lnuqq_ATLAS13 |
| class | Hobs_gg_phi3_Zga_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to Z\gamma\). More... | |
| class | Hobs_gg_phi3_Zga_llga_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to Z\gamma\). More... | |
| class | Hobs_gg_phi3_Zga_qqga_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to Z\gamma\). More... | |
| class | Hobs_gg_phi3_ZZ_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg \to \phi_{3}\to ZZ\). More... | |
| class | Hobs_gg_phi3_ZZ_llllnunu_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to ZZ\). More... | |
| class | Hobs_gg_phi3_ZZ_llnunuqq_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to ZZ\). More... | |
| class | Hobs_ggVV_phi2_WW_lnulnu_CMS13 |
| class | Hobs_ggVV_phi3_WW_lnulnu_CMS13 |
| class | Hobs_mu_pp_phi2_VV_CMS8 |
| Ratio of the prediction and CMS upper limit for the signal strength of the process \(pp \to \phi_{2}\to VV\). More... | |
| class | Hobs_mu_pp_phi3_VV_CMS8 |
| Ratio of the prediction and CMS upper limit for the signal strength of the process \(pp \to \phi_{3}\to VV\). More... | |
| class | Hobs_pp_Hp_taunu_CMS8_GTHDM |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio. More... | |
| class | Hobs_pp_Hp_tb_CMS8_GTHDM |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to AZ\to \tau\tau\ell\ell\). More... | |
| class | Hobs_pp_Hpm_taunu_ATLAS13_GTHDM |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to AZ\to \tau\tau\ell\ell\). More... | |
| class | Hobs_pp_Hpm_taunu_ATLAS8_GTHDM |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio. More... | |
| class | Hobs_pp_Hpm_taunu_CMS13_GTHDM |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to AZ\to \tau\tau\ell\ell\). More... | |
| class | Hobs_pp_Hpm_tb_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to AZ\to \tau\tau\ell\ell\). More... | |
| class | Hobs_pp_Hpm_tb_ATLAS8_GTHDM |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to AZ\to \tau\tau\ell\ell\). More... | |
| class | Hobs_pp_phi2_bb_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to b\bar b\). More... | |
| class | Hobs_pp_phi2_gaga_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \gamma \gamma\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbbb_1_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b b\bar b\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbbb_2_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b b\bar b\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbbb_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b b\bar b\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbbb_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp \to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b b\bar b\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbgaga_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbgaga_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to bb \gamma \gamma\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbgaga_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp \to \phi_{2}\to \phi_{1}\phi_{1}\to \gamma\gamma b\bar b\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbtautau_1_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbtautau_2_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbtautau_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b \tau \tau\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbtautau_CMS8 |
| class | Hobs_pp_phi2_phi1phi1_bbVV_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1}\to b\bar b VV\to b\bar b \ell \ell \nu \nu\). More... | |
| class | Hobs_pp_phi2_phi1phi1_bbWW_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{1}\phi_{1} [\to b\bar b WW]\). More... | |
| class | Hobs_pp_phi2_phi3Z_bbll_1_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to AZ\to b\bar b \ell\ell\). More... | |
| class | Hobs_pp_phi2_phi3Z_bbll_2_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to AZ\to b\bar b \ell\ell\). More... | |
| class | Hobs_pp_phi2_phi3Z_tautaull_1_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to \phi_{3}Z\to \tau\tau\ell\ell\). More... | |
| class | Hobs_pp_phi2_phi3Z_tautaull_2_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to AZ\to \tau\tau\ell\ell\). More... | |
| class | Hobs_pp_phi2_VV_qqqq_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to WW,ZZ\). More... | |
| class | Hobs_pp_phi2_WW_lnuqq_CMS13 |
| class | Hobs_pp_phi2_Zga_llga_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to Z\gamma\). More... | |
| class | Hobs_pp_phi2_Zga_llga_CMS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to Z\gamma\). More... | |
| class | Hobs_pp_phi2_ZZ_llqqnunull_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{2}\to ZZ\). More... | |
| class | Hobs_pp_phi2_ZZ_qqnunu_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to ZZ\). More... | |
| class | Hobs_pp_phi3_bb_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to b\bar b\). More... | |
| class | Hobs_pp_phi3_gaga_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \gamma \gamma\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbbb_1_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b b\bar b\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbbb_2_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b b\bar b\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbbb_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b b\bar b\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbbb_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp \to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b b\bar b\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbgaga_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbgaga_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to bb \gamma \gamma\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbgaga_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp \to \phi_{3}\to \phi_{1}\phi_{1}\to \gamma\gamma b\bar b\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbtautau_1_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \to b\bar b \tau \tau\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbtautau_2_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \to b\bar b \tau \tau\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbtautau_ATLAS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \to b\bar b \tau \tau\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbtautau_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp \to \phi_{3}\to \phi_{1}\phi_{1}\to \tau\tau b\bar b\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbVV_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1}\to b\bar b VV\to b\bar b \ell \ell \nu \nu\). More... | |
| class | Hobs_pp_phi3_phi1phi1_bbWW_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{1}\phi_{1} [\to b\bar b WW]\). More... | |
| class | Hobs_pp_phi3_phi2Z_bbll_1_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to AZ\to b\bar b \ell\ell\). More... | |
| class | Hobs_pp_phi3_phi2Z_bbll_2_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to AZ\to b\bar b \ell\ell\). More... | |
| class | Hobs_pp_phi3_phi2Z_tautaull_1_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{2}Z\to \tau\tau\ell\ell\). More... | |
| class | Hobs_pp_phi3_phi2Z_tautaull_2_CMS8 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to \phi_{2}Z\to \tau\tau\ell\ell\). More... | |
| class | Hobs_pp_phi3_VV_qqqq_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to WW,ZZ\). More... | |
| class | Hobs_pp_phi3_WW_lnuqq_CMS13 |
| class | Hobs_pp_phi3_Zga_llga_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to Z\gamma\). More... | |
| class | Hobs_pp_phi3_Zga_llga_CMS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to Z\gamma\). More... | |
| class | Hobs_pp_phi3_ZZ_llqqnunull_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(pp\to \phi_{3}\to ZZ\). More... | |
| class | Hobs_pp_phi3_ZZ_qqnunu_CMS13 |
| Ratio of the prediction and CMS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to ZZ\). More... | |
| class | Hobs_tt_phi2_tt_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(t\bar t \to \phi_{2}\to t\bar t\). More... | |
| class | Hobs_tt_phi3_tt_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(t\bar t \to \phi_{3}\to t\bar t\). More... | |
| class | Hobs_VV_phi2_WW_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(VV \to \phi_{2}\to WW\). More... | |
| class | Hobs_VV_phi2_WW_enumunu_ATLAS13 |
| class | Hobs_VV_phi2_WW_lnuqq_ATLAS13 |
| class | Hobs_VV_phi2_ZZ_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(VV \to \phi_{2}\to ZZ\). More... | |
| class | Hobs_VV_phi2_ZZ_llllnunu_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(VV\to \phi_{2}\to ZZ\). More... | |
| class | Hobs_VV_phi2_ZZ_llnunuqq_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{2}\to ZZ\). More... | |
| class | Hobs_VV_phi3_WW_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(VV \to \phi_{3}\to WW\). More... | |
| class | Hobs_VV_phi3_WW_enumunu_ATLAS13 |
| class | Hobs_VV_phi3_WW_lnuqq_ATLAS13 |
| class | Hobs_VV_phi3_ZZ_ATLAS8 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(VV \to \phi_{3}\to ZZ\). More... | |
| class | Hobs_VV_phi3_ZZ_llllnunu_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(VV\to \phi_{3}\to ZZ\). More... | |
| class | Hobs_VV_phi3_ZZ_llnunuqq_ATLAS13 |
| Ratio of the prediction and ATLAS upper limit for the cross section times branching ratio of the process \(gg\to \phi_{3}\to ZZ\). More... | |
| class | Imlambda5H_GTHDM |
| parameter of the Higgs potential \(\Im\lambda_{5}\) in the Higgs basis More... | |
| class | Imlambda6H_GTHDM |
| parameter of the Higgs potential \(\Im\lambda_{6}\) in the Higgs basis More... | |
| class | Imlambda7H_GTHDM |
| parameter of the Higgs potential \(\Im\lambda_{7}\) in the Higgs basis More... | |
| class | Imm12_2_GTHDM |
| parameter of the Higgs potential \(Im(m_{12}^2)\) More... | |
| class | lambda1_GTHDM |
| parameter of the Higgs potential \(\lambda_{1}\) More... | |
| class | lambda1atQGTHDM |
| lambda1atQGTHDM. More... | |
| class | lambda1H_GTHDM |
| parameter of the Higgs potential \(\lambda_{1}\) in the Higgs basis More... | |
| class | lambda2_GTHDM |
| parameter of the Higgs potential \(\lambda_{2}\) More... | |
| class | lambda2atQGTHDM |
| lambda2atQGTHDM. More... | |
| class | lambda2H_GTHDM |
| parameter of the Higgs potential \(\lambda_{2}\) in the Higgs basis More... | |
| class | lambda3_GTHDM |
| parameter of the Higgs potential \(\lambda_{3}\) More... | |
| class | lambda3atQGTHDM |
| lambda3atQGTHDM. More... | |
| class | lambda3H_GTHDM |
| parameter of the Higgs potential \(\lambda_{3}\) in the Higgs basis More... | |
| class | lambda4_GTHDM |
| parameter of the Higgs potential \(\lambda_{4}\) More... | |
| class | lambda4atQGTHDM |
| lambda4atQGTHDM. More... | |
| class | lambda4H_GTHDM |
| parameter of the Higgs potential \(\lambda_{4}\) in the Higgs basis More... | |
| class | log10_bb_phi2_bb_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(pp\to \phi_{2}\to b\bar b\) at 13 TeV. More... | |
| class | log10_bb_phi2_bb_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(b\bar b\to \phi_{2}\to b\bar b\) at 8 TeV. More... | |
| class | log10_bb_phi2_tautau_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(b\bar b\to \phi_{2}\to \tau \tau\) at 13 TeV. More... | |
| class | log10_bb_phi2_tautau_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(b\bar b\to \phi_{2}\to \tau\tau\) at 8 TeV. More... | |
| class | log10_bb_phi2_tt_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(b\bar b\to \phi_{2}\to t\bar t\) at 13 TeV. More... | |
| class | log10_bb_phi3_bb_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(pp\to \phi_{3}\to b\bar b\) at 13 TeV. More... | |
| class | log10_bb_phi3_bb_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(b\bar b\to \phi_{3}\to b\bar b\) at 8 TeV. More... | |
| class | log10_bb_phi3_tautau_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(b\bar b\to \phi_{3}\to \tau \tau\) at 13 TeV. More... | |
| class | log10_bb_phi3_tautau_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(b\bar b\to \phi_{3}\to \tau\tau\) at 8 TeV. More... | |
| class | log10_bb_phi3_tt_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(b\bar b\to \phi_{3}\to t\bar t\) at 13 TeV. More... | |
| class | log10_gg_phi2_bb_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(b\bar b\to \phi_{2}\to b\bar b\) at 8 TeV. More... | |
| class | log10_gg_phi2_gaga_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{2}\to \gamma \gamma\) at 13 TeV. More... | |
| class | log10_gg_phi2_gaga_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{2}\to \gamma\gamma\) at 8 TeV. More... | |
| class | log10_gg_phi2_tautau_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{2}\to \tau \tau\) at 13 TeV. More... | |
| class | log10_gg_phi2_tautau_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{2}\to \tau\tau\) at 8 TeV. More... | |
| class | log10_gg_phi2_WW_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{2}\to WW\) at 13 TeV. More... | |
| class | log10_gg_phi2_WW_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{2}\to WW\) at 8 TeV. More... | |
| class | log10_gg_phi2_Zga_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{2}\to Z\gamma\) at 13 TeV. More... | |
| class | log10_gg_phi2_ZZ_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{2}\to ZZ\) at 13 TeV. More... | |
| class | log10_gg_phi2_ZZ_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{2}\to ZZ\) at 8 TeV. More... | |
| class | log10_gg_phi3_bb_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(b\bar b\to \phi_{3}\to b\bar b\) at 8 TeV. More... | |
| class | log10_gg_phi3_gaga_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{3}\to \gamma \gamma\) at 13 TeV. More... | |
| class | log10_gg_phi3_gaga_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{3}\to \gamma\gamma\) at 8 TeV. More... | |
| class | log10_gg_phi3_tautau_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{3}\to \tau \tau\) at 13 TeV. More... | |
| class | log10_gg_phi3_tautau_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{3}\to \tau\tau\) at 8 TeV. More... | |
| class | log10_gg_phi3_WW_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{3}\to WW\) at 13 TeV. More... | |
| class | log10_gg_phi3_WW_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{3}\to WW\) at 8 TeV. More... | |
| class | log10_gg_phi3_Zga_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{3}\to Z\gamma\) at 13 TeV. More... | |
| class | log10_gg_phi3_ZZ_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{3}\to ZZ\) at 13 TeV. More... | |
| class | log10_gg_phi3_ZZ_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(gg\to \phi_{3}\to ZZ\) at 8 TeV. More... | |
| class | log10_ggVV_phi2_WW_lnulnu_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \((gg+VV)\to \phi_{2}\to WW\to \ell \nu \ell \nu\) at 13 TeV. More... | |
| class | log10_ggVV_phi3_WW_lnulnu_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \((gg+VV)\to \phi_{3}\to WW\to \ell \nu \ell \nu\) at 13 TeV. More... | |
| class | log10_pp_phi2_bb_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(pp\to \phi_{2}\to b\bar b\) at 13 TeV. More... | |
| class | log10_pp_phi2_gaga_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(pp\to \phi_{2}\to \gamma \gamma\) at 13 TeV. More... | |
| class | log10_pp_phi2_WW_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \((pp)\to \phi_{2}\to WW \) at 13 TeV. More... | |
| class | log10_pp_phi2_Zga_llga_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(pp\to \phi_{2}\to Z\gamma \to \ell \ell \gamma\) at 8 TeV. More... | |
| class | log10_pp_phi2_ZZ_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(pp\to \phi_{2}\to ZZ\) at 13 TeV. More... | |
| class | log10_pp_phi3_bb_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(pp\to \phi_{3}\to b\bar b\) at 13 TeV. More... | |
| class | log10_pp_phi3_gaga_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(pp\to \phi_{3}\to \gamma \gamma\) at 13 TeV. More... | |
| class | log10_pp_phi3_Zga_llga_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(pp\to \phi_{3}\to Z\gamma \to \ell \ell \gamma\) at 8 TeV. More... | |
| class | log10_pp_phi3_ZZ_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(pp\to \phi_{3}\to ZZ\) at 13 TeV. More... | |
| class | log10_tt_phi2_tt_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(t\bar t\to \phi_{2}\to t\bar t\) at 13 TeV. More... | |
| class | log10_tt_phi3_tt_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(t\bar t\to \phi_{3}\to t\bar t\) at 13 TeV. More... | |
| class | log10_VV_phi2_WW_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(VV\to \phi_{2}\to WW\) at 13 TeV. More... | |
| class | log10_VV_phi2_WW_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(VV\to \phi_{2}\to WW\) at 8 TeV. More... | |
| class | log10_VV_phi2_ZZ_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(VV\to \phi_{2}\to ZZ\) at 13 TeV. More... | |
| class | log10_VV_phi2_ZZ_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(VV\to \phi_{2}\to ZZ\) at 8 TeV. More... | |
| class | log10_VV_phi3_WW_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(VV\to \phi_{3}\to WW\) at 13 TeV. More... | |
| class | log10_VV_phi3_WW_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(VV\to \phi_{3}\to WW\) at 8 TeV. More... | |
| class | log10_VV_phi3_ZZ_TH13 |
| Decadic logarithm of the cross section times branching ratio of the process \(VV\to \phi_{3}\to ZZ\) at 13 TeV. More... | |
| class | log10_VV_phi3_ZZ_TH8 |
| Decadic logarithm of the cross section times branching ratio of the process \(VV\to \phi_{3}\to ZZ\) at 8 TeV. More... | |
| class | m11_2_GTHDM |
| parameter of the Higgs potential \(m_{11}^2\) More... | |
| class | m1_2 |
| class | m22_2_GTHDM |
| parameter of the Higgs potential \(m_{22}^2\) More... | |
| class | m2_2 |
| class | M2_GTHDM |
| parameter of the Higgs potential \(M^2\) More... | |
| class | m3_2 |
| class | mH1_2 |
| The mass of the SM Higgs. More... | |
| class | mH1_GTHDM |
| The mass of the SM Higgs. More... | |
| class | mH1sq_GTHDM |
| The SM Higgs mass squared. More... | |
| class | mH2_2 |
| The mass of the SM Higgs. More... | |
| class | mH2_GTHDM |
| The mass of the second neutral Higgs. More... | |
| class | mH2mmH1_GTHDM |
| The mass difference between the second neutral Higgs and the SM Higgs. More... | |
| class | mH2mmHp_GTHDM |
| The mass difference between the second neutral Higgs and the charged Higgs. More... | |
| class | mH2sq_GTHDM |
| The second neutral Higgs mass squared. More... | |
| class | mH3_2 |
| The mass of the SM Higgs. More... | |
| class | mH3_GTHDM |
| The mass of the third neutral Higgs. More... | |
| class | mH3mmH1_GTHDM |
| The mass difference between the third neutral Higgs and the SM Higgs. More... | |
| class | mH3mmH2_GTHDM |
| The mass difference between the third and the second neutral Higgs. More... | |
| class | mH3mmHp_GTHDM |
| The mass difference between the third neutral Higgs and the charged Higgs. More... | |
| class | mH3sq_GTHDM |
| The third neutral Higgs mass squared. More... | |
| class | mHheavy_GTHDM |
| The mass of the heaviest neutral Higgs. More... | |
| class | mHlight_GTHDM |
| The mass of the lightest neutral Higgs. More... | |
| class | mHmedium_GTHDM |
| The mass of the medium-weighted neutral Higgs. More... | |
| class | mHp_GTHDM |
| The mass of the charged Higgs. More... | |
| class | mHpmmH1_GTHDM |
| The mass difference between the charged Higgs and the SM Higgs. More... | |
| class | Msq11_GTHDM |
| The (1,1) entry of the non-diagonal neutral Higgs mass square matrix. More... | |
| class | Msq12_GTHDM |
| The (1,2) entry of the non-diagonal neutral Higgs mass square matrix. More... | |
| class | Msq13_GTHDM |
| The (1,3) entry of the non-diagonal neutral Higgs mass square matrix. More... | |
| class | Msq22_GTHDM |
| The (2,2) entry of the non-diagonal neutral Higgs mass square matrix. More... | |
| class | Msq23_GTHDM |
| The (2,3) entry of the non-diagonal neutral Higgs mass square matrix. More... | |
| class | Msq33_GTHDM |
| The (3,3) entry of the non-diagonal neutral Higgs mass square matrix. More... | |
| class | Q_stGTHDM |
| Q_stTHDMW. More... | |
| class | R11_GTHDM |
| Element (1,1) of the ortogonal matrix determining the mass e/states. More... | |
| class | R12_GTHDM |
| Element (1,2) of the ortogonal matrix determining the mass e/states. More... | |
| class | R13_GTHDM |
| Element (1,3) of the ortogonal matrix determining the mass e/states. More... | |
| class | R22_GTHDM |
| Element (2,2) of the ortogonal matrix determining the mass e/states. More... | |
| class | R23_GTHDM |
| Element (2,3) of the ortogonal matrix determining the mass e/states. More... | |
| class | R31_GTHDM |
| Element (3,1) of the ortogonal matrix determining the mass e/states. More... | |
| class | R32_GTHDM |
| Element (3,2) of the ortogonal matrix determining the mass e/states. More... | |
| class | R33_GTHDM |
| Element (3,3) of the ortogonal matrix determining the mass e/states. More... | |
| class | Rb0 |
| class | Relambda5atQGTHDM |
| Relambda5atQGTHDM. More... | |
| class | Relambda5H_GTHDM |
| parameter of the Higgs potential \(\Re\lambda_{5}\) in the Higgs basis More... | |
| class | Relambda6atQGTHDM |
| Relambda6atQGTHDM. More... | |
| class | Relambda6H_GTHDM |
| parameter of the Higgs potential \(\Re\lambda_{6}\) in the Higgs basis More... | |
| class | Relambda7atQGTHDM |
| Relambda7atQGTHDM. More... | |
| class | Relambda7H_GTHDM |
| parameter of the Higgs potential \(\Re\lambda_{7}\) in the Higgs basis More... | |
| class | Rem12_2_GTHDM |
| parameter of the Higgs potential \(Re(m_{12}^2)\) More... | |
| class | Resigmau |
| Real part of the up-type Yukawa coupling parameter sigma. More... | |
| class | rh_gaga_GTHDM |
| Squared relative coupling of \(h\) to two photons. More... | |
| class | rh_gg_GTHDM |
| Squared relative coupling of \(h\) to two gluons. More... | |
| class | rh_Zga_GTHDM |
| Squared relative coupling of \(h\) to a Z and a photon. More... | |
| class | sdR_GTHDM |
| Real part of Yukawa down coupling. More... | |
| class | slR_GTHDM |
| Real part of Yukawa leptonic coupling. More... | |
| class | suR_GTHDM |
| Real part Yukawa up coupling. More... | |
| class | tanbeta_GTHDM |
| The tangent of beta. More... | |
| class | v1_GTHDM |
| The vacuum expectation value of \(\Phi_1\) in the generic basis. More... | |
| class | v2_GTHDM |
| The vacuum expectation value of \(\Phi_2\) in the generic basis. More... | |
| class | yd1R_GTHDM |
| Coupling of the SM-Higgs to down quarks real part. More... | |
| class | yl1R_GTHDM |
| Coupling of the SM-Higgs to leptons real part. More... | |
| class | yu1R_GTHDM |
| Coupling of the SM-Higgs to up quarks real part. More... | |
A module for general Two-Higgs-Doublet models (without the assumption of a \(Z_2\) symmetry).
This module contains code necessary for analyzing theoretical and experimental constraints on general symmetric Two-Higgs-Doublet models. While the theoretical bounds (positivity, unitarity and stability of the Higgs potential) as well as the electroweak STU pseudo-observables are available in the most general case, the Higgs and flavour observables are currently only implemented in the flavour aligned limiting case.