We report the recent progress in understanding of symmetries which can be implemented in the scalar sector of electroweak symmetry breaking models with several Higgs doublets. In particular we present the list of finite reparametrization symmetry groups which can appear in the three-Higgs-doublet models.
Making use of a dimensionally-reduced effective theory at high temperature, we perform a nonperturbative study of the electroweak phase transition in the Two Higgs Doublet model. We focus on two phenomenologically allowed points in the parameter space, carrying out dynamical lattice simulations to determine the equilibrium properties of the transition. We discuss the shortcomings of conventional perturbative approaches based on the resummed effective potential -regarding the insufficient handling of infrared resummation but also the need to account for corrections beyond 1-loop order in the presence of large scalar couplings -and demonstrate that greater accuracy can be achieved with perturbative methods within the effective theory. We find that in the presence of very large scalar couplings, strong phase transitions cannot be reliably studied with any of the methods. arXiv:1904.01329v2 [hep-ph] 24 Jun 2019 7 Conclusions 27 A Renormalization in the MS scheme 29 -1 -redefinition of µ 2 12 and λ5 and renders the model CP conserving. 3 The Type-X and Type-Y 2HDMs are also referred to as the lepton-specific and flipped 2HDMs, respectively [19].
In non-minimal Higgs mechanisms, one often needs to minimize highly symmetric
Higgs potentials. Here we propose a geometric way of doing it, which,
surprisingly, is often much more efficient than the usual method. By
construction, it gives the global minimum for any set of free parameters of the
potential, thus offering an intuitive understanding of how they affect the
vacuum expectation values. For illustration, we apply this method to the S_4
and A_4-symmetric three-Higgs-doublet models. We find that at least three
recent phenomenological analyses of the A_4-symmetric model used a local, not
the global minimum. We discuss coexistence of minima of different types, and
comment on the mathematical origin of geometrical CP-violation and on a new
symmetry linking different minima.Comment: 18 pages, 3 figures; v2: corrected comments on Ref.[7]; v3: minor
modifications, matches the published versio
Following the discovery of a Higgs boson, there has been renewed interest in the general 2-Higgs-Doublet Model (2HDM). A model with One Inert Doublet plus One Higgs Doublet (I(1+1)HDM), where one of the scalar doublets is "inert" (since it has no vacuum expectation value and does not couple to fermions) has an advantage over the 2HDM since it provides a good Dark Matter (DM) candidate, namely the lightest inert scalar. Motivated by the existence of three fermion families, here we consider a model with two scalar doublets plus one Higgs doublet (I(2+1)HDM), where the two scalar doublets are inert. The I(2+1)HDM has a richer phenomenology than either the I(1+1)HDM or the 2HDM. We discuss the new regions of DM relic density in the I(2+1)HDM with simplified couplings and address the possibility of constraining the model using recent results from the Large Hadron Collider (LHC) and DM direct detection experiments.
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