Abstract
In multi-Higgs models, the properties of one neutral scalar state approximate those of the Standard Model (SM) Higgs boson in a limit where the corresponding scalar field is roughly aligned in field space with the scalar doublet vacuum expectation value. In a scenario of alignment without decoupling, a SM-like Higgs boson can be accompanied by additional scalar states whose masses are of a similar order of magnitude. In the Minimal Supersymmetric Standard Model (MSSM), alignment without decoupling can be achieved due to an accidental cancellation of tree-level and radiative loop-level effects. In this paper we assess the impact of the leading two-loop mathcal{O}(alpha _s h_t^2) corrections on the Higgs alignment condition in the MSSM. These corrections are sizable and important in the relevant regions of parameter space and furthermore give rise to solutions of the alignment condition that are not present in the approximate one-loop description. We provide a comprehensive numerical comparison of the alignment condition obtained in the approximate one-loop and two-loop approximations, and discuss its implications for phenomenologically viable regions of the MSSM parameter space.
Highlights
Deviations from the Standard Model (SM) Higgs behavior can be accommodated by introducing additional Higgs scalars to the electroweak model
Given the current precision of Higgs boson measurements at the Large Hadron Collider (LHC), the observed state with mass 125 GeV is consistent with a Higgs boson that possesses the spin, CP quantum number and coupling properties predicted by the SM
In an extended Higgs sector of a beyond the SM (BSM) theory, a scalar mass eigenstate would possess the properties of the SM Higgs boson if it is aligned in field space with the scalar vacuum expectation value responsible for electroweak symmetry breaking
Summary
Deviations from the SM Higgs behavior can be accommodated by introducing additional Higgs scalars to the electroweak model. In any multi-Higgs doublet model, an exact alignment condition can be specified, in which the aligned scalar field is a mass eigenstate (and its mixing with all other scalar eigenstate fields vanishes) If this alignment condition is approximately fulfilled, it is possible to have a SM-like Higgs boson along with additional scalar states with masses that are not significantly larger than the electroweak scale and more amenable to discovery in future LHC runs. We denote the latter scenario alignment without decoupling [4–8, 12–14].
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