Abstract

We study the Higgs mass spectrum as predicted by a Maximally Symmetric Two Higgs Doublet Model (MS-2HDM) potential based on the SO(5) group, softly broken by bilinear Higgs mass terms. We show that the lightest Higgs sector resulting from this MS-2HDM becomes naturally aligned with that of the Standard Model (SM), independently of the charged Higgs boson mass and $\tan \beta$. In the context of Type-II 2HDM, SO(5) is the simplest of the three possible symmetry realizations of the scalar potential that can naturally lead to the SM alignment. Nevertheless, renormalization group effects due to the hypercharge gauge coupling $g'$ and third-generation Yukawa couplings may break sizeably this SM alignment, along with the custodial symmetry inherited by the SO(5) group. Using the current Higgs signal strength data from the LHC, which disfavour large deviations from the SM alignment limit, we derive lower mass bounds on the heavy Higgs sector as a function of $\tan\beta$, which can be stronger than the existing limits for a wide range of parameters. In particular, we propose a new collider signal based on the observation of four top quarks to directly probe the heavy Higgs sector of the MS-2HDM during the run-II phase of the LHC.

Highlights

  • Which contains four real mass parameters μ21,2, Re(m212), Im(m212), and ten real quartic couplings λ1,2,3,4, Re(λ5,6,7), and Im(λ5,6,7)

  • We show that the lightest Higgs sector resulting from this Maximally Symmetric 2HDM (MS-2HDM) becomes naturally aligned with that of the Standard Model (SM), independently of the charged Higgs boson mass and tan β

  • We have analyzed the symmetries of the 2HDM scalar potential to naturally justify the so-called SM alignment limit, independently of the heavy Higgs spectrum and the value of tan β

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Summary

Maximally symmetric two Higgs doublet model potential

In order to identify all accidental symmetries of the 2HDM potential, it is convenient to introduce the 8-dimensional complex multiplet [7, 28, 29]: Φ1. We may identify all maximal symmetries of the 2HDM potential by classifying all proper, improper and semi-simple subgroups of SO(5) in the bilinear RI space. In this way, it was found [7, 29] that a 2HDM potential invariant under SU(2)L ⊗ U(1)Y can possess a maximum of 13 accidental symmetries. Even in the custodial symmetric limit g → 0, the latter only possesses a smaller symmetry: O(2) ⊗ O(3) ⊂ SO(5), in the 5-dimensional bilinear RI space

Custodial symmetries in the MS-2HDM
Scalar spectrum in the MS-2HDM
RG and soft breaking effects
Misalignment predictions
Collider signals
Branching fractions
Charged Higgs signal
Heavy neutral Higgs signal
Conclusions
A Higgs spectrum and couplings in a general 2HDM
Findings
B Two-loop RGEs in a general 2HDM
Full Text
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