A search for exotic decays of the Higgs boson (H) with a mass of 125 GeV to a pair of light pseudoscalars a1 is performed in final states where one pseudoscalar decays to two b quarks and the other to a pair of muons or τ leptons. A data sample of proton–proton collisions at √s = 13 TeV cor- responding to an integrated luminosity of 138 fb−1 recorded with the CMS detector is analyzed. No statistically signifi- cant excess is observed over the standard model backgrounds. Upper limits are set at 95% confidence level (CL) on the Higgs boson branching fraction to μμbb and to ττbb, via a pair of a1 s. The limits depend on the pseudoscalar mass ma1 and are observed to be in the range (0.17–3.3) ×10−4 and (1.7–7.7) ×10−2 in the μμbb and ττbb final states, respec- tively. In the framework of models with two Higgs doublets and a complex scalar singlet (2HDM+S), the results of the two final states are combined to determine upper limits on the branching fraction B(H → a1 a 1 → bb) at 95% CL, with being a muon or a τ lepton. For different types of 2HDM+S, upper bounds on the branching fraction B(H → a 1 a1) are extracted from the combination of the two channels. In most of the Type II 2HDM+S parameter space, B(H → a 1 a1) values above 0.23 are excluded at 95% CL for ma1 values between 15 and 60 GeV

Search for exotic decays of the Higgs boson to a pair of pseudoscalars in the mu mu b b and tau tau b b final states

CANDELISE, V.;DE LEO, K.;DELLA RICCA, G.;
2024-01-01

Abstract

A search for exotic decays of the Higgs boson (H) with a mass of 125 GeV to a pair of light pseudoscalars a1 is performed in final states where one pseudoscalar decays to two b quarks and the other to a pair of muons or τ leptons. A data sample of proton–proton collisions at √s = 13 TeV cor- responding to an integrated luminosity of 138 fb−1 recorded with the CMS detector is analyzed. No statistically signifi- cant excess is observed over the standard model backgrounds. Upper limits are set at 95% confidence level (CL) on the Higgs boson branching fraction to μμbb and to ττbb, via a pair of a1 s. The limits depend on the pseudoscalar mass ma1 and are observed to be in the range (0.17–3.3) ×10−4 and (1.7–7.7) ×10−2 in the μμbb and ττbb final states, respec- tively. In the framework of models with two Higgs doublets and a complex scalar singlet (2HDM+S), the results of the two final states are combined to determine upper limits on the branching fraction B(H → a1 a 1 → bb) at 95% CL, with being a muon or a τ lepton. For different types of 2HDM+S, upper bounds on the branching fraction B(H → a 1 a1) are extracted from the combination of the two channels. In most of the Type II 2HDM+S parameter space, B(H → a 1 a1) values above 0.23 are excluded at 95% CL for ma1 values between 15 and 60 GeV
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11368/3074978
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