Explanation of the excesses in associated di-photon production at 152 GeV in 2HDM

Abstract

Statistically significant excesses exist at around 152 GeV in associated di-photon production ($\gamma \gamma +X$) in the sidebands of SM Higgs analyses of ATLAS (using the full run-2 dataset). They are most pronounced in the single-$\tau$, missing-transverse-energy, four-jet and $⩾1\ell +⩾1b$-jet channels ($\approx 3\sigma$) and can be explained by the Drell-Yan production of new Higgs bosons, i.e. $pp\to W^{\ast }\to H^{\pm }{H}^0$. We first examine the excesses in a simplified model approach, considering that $H^{\pm }$ decays to $\tau \nu$, $WZ$ or $tb$. Both the $\tau \nu$ and $tb$ decay modes individually lead to a significance of $⪅4\sigma$ while for $WZ$ one can obtain at most $3.5\sigma$. This is because the decays of $WZ$ lead to multiple leptons contributing to the two-lepton channel which does not show an excess at 152 GeV. Next, we consider two-Higgs-doublet models where the charged Higgs does not decay to $WZ$ at tree-level, finding a significance of $⪆4\sigma$ for a branching ratio of the new neutral Higgs to photons of $\approx$2%. Even though this branching fraction is quite sizable, it can be obtained in composite models or via the Lagrangian term ${\lambda }_6{H}_1^{†}{H}_1{H}_2^{†}{H}_1+h.c.$ breaking the commonly imposed $Z_2$ symmetry.

Comments: 12 pages, 5 figures, version accepted for publication in JHEP