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Two-Higgs-doublet type-II and -III models and $$t\rightarrow c h$$ at the LHC
Authors:A?Arhrib  Email author" target="_blank">R?BenbrikEmail author  Chuan-Hung?Chen  Melina?Gomez-Bock  Souad?Semlali
Institution:1.Département de Mathématiques, Faculté des Sciences et Techniques,Université Abdelmalek Essaadi,Tangier,Morocco;2.Physics Division,National Center for Theoretical Sciences,Hsinchu,Taiwan;3.LPHEA, Semlalia,Cadi Ayyad University,Marrakech,Morocco;4.MSISM Team,Faculté Polydisciplinaire de Safi,Safi,Morocco;5.Department of Physics,National Cheng-Kung University,Tainan,Taiwan;6.DAFM,Universidad de las Américas Puebla,Cholula,Mexico
Abstract:We study the constraints of the generic two-Higgs-doublet model (2HDM) type-III and the impacts of the new Yukawa couplings. For comparisons, we revisit the analysis in the 2HDM type-II. To understand the influence of all involving free parameters and to realize their correlations, we employ a \(\chi \)-square fitting approach by including theoretical and experimental constraints, such as the S, T, and U oblique parameters, the production of standard model Higgs and its decay to \(\gamma \gamma \), \(WW^*/ZZ^*\), \(\tau ^+\tau ^-\), etc. The errors of the analysis are taken at 68, 95.5, and \(99.7~\%\) confidence levels. Due to the new Yukawa couplings being associated with \(\cos (\beta -\alpha )\) and \(\sin (\beta -\alpha )\), we find that the allowed regions for \(\sin \alpha \) and \(\tan \beta \) in the type-III model can be broader when the dictated parameter \(\chi _F\) is positive; however, for negative \(\chi _F\), the limits are stricter than those in the type-II model. By using the constrained parameters, we find that the deviation from the SM in \(h\rightarrow Z\gamma \) can be of \(\mathcal{O}(10~\%)\). Additionally, we also study the top-quark flavor-changing processes induced at the tree level in the type-III model and find that when all current experimental data are considered, we get \(Br(t\rightarrow c(h, H) )< 10^{-3}\) for \(m_h=125.36\) and \(m_H=150\) GeV, and \(Br(t\rightarrow cA)\) slightly exceeds \(10^{-3}\) for \(m_A =130\) GeV.
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