Abstract
If the Higgs boson decays to a pair of invisible particles, the number of di-Higgs events, where each Higgs decay into Standard Model (SM) particles, are reduced by a factor of two-third taking into account the current LHC bound on invisible decay width of the Higgs boson. We investigate the sensitivity of the upcoming high luminosity run of the LHC to di-Higgs production and subsequent decay to dark matter in the context of the singlet scalar extension of the SM augmented by a fermionic dark matter in the dark and bright channel $\gamma\gamma+\not\!\! E_T$. Once systematic uncertainties on background yields are considered, this dark and bright channel presents competitive limits than $b\bar{b}+\not\!\! E_T$ after a careful tuning of the kinematical cuts that raise the signal over background ratio. We further show that in a multivariate analysis, for an invisible branching fraction as low as $\sim 10$%, we obtain stronger bounds for the Higgs trilinear coupling from the $\gamma\gamma+\not\!\! E_T$ channel compared to the $b\bar{b}\gamma\gamma$ final state. Finally, we demonstrate that the three channels $\gamma\gamma+\not\!\! E_T$, $b\bar{b}+\not\!\! E_T$ and $b\bar{b}\gamma\gamma$, complement each other in the search for di-Higgs production with non-SM trilinear couplings when an invisible decay mode is present.
Highlights
After the discovery of the Higgs boson at the LHC [1,2], and the confirmation that this spin-0 particle plays a role in the electroweak symmetry breaking (EWSB) mechanism [3,4,5], the LHC still has a long road to unravel the details of the Higgs boson self-interactions by measuring its trilinear and quartic couplings
We investigate the sensitivity of the upcoming high luminosity run of the LHC to di-Higgs production and subsequent decay to dark matter in the context of the singlet scalar extension of the Standard Model (SM) augmented by a fermionic dark matter in the dark and bright channel γγ þ ET
The production of two Higgs bosons is of prime importance to understand the scalar sector of the Standard Model
Summary
After the discovery of the Higgs boson at the LHC [1,2], and the confirmation that this spin-0 particle plays a role in the electroweak symmetry breaking (EWSB) mechanism [3,4,5], the LHC still has a long road to unravel the details of the Higgs boson self-interactions by measuring its trilinear and quartic couplings. We focus on the part of the xSM parameters space that respects several experimental and theoretical constraints, and where new heavy Higgs bosons are not expected to be observable at the LHC but shift the SM Higgs trilinear coupling away from its SM value. In this case, our results can be useful to constrain other models with non-SM trilinear couplings.
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