Measurements of properties of the Higgs boson decaying into the four . . . Properties of the Higgs boson are measured in the H to ZZ to 4l (l= e, mu) decay channel A data sample of proton-proton collisions at sqrt (s) = 13 TeV, collected with the CMS detector at the LHC and corresponding to an integrated luminosity of 35 9 inverse femtobarns is used
Measurements of properties of the Higgs boson decaying into the four . . . Abstract Properties of the Higgs boson are measured in the H → ZZ → 4ℓ (ℓ = e, μ) decay channel A data sample of proton-proton collisions at √s = 13 TeV, collected with the CMS detector at the LHC and corresponding to an integrated luminosity of 35 9 fb⁻¹ is used
Measurements of properties of the Higgs boson decaying into the four . . . Properties of the Higgs boson are measured in the H → ZZ → 4ℓ (ℓ = e, μ) decay channel A data sample of proton-proton collisions at $ \sqrt {s}=13 $ TeV, collected with the CMS detector at the LHC and corresponding to an integrated luminosity of 35 9 fb$^ {−1}$ is used
Measurements of properties of the Higgs boson decaying into the four . . . The signal strength modifier μ, defined as the ratio of the observed Higgs boson rate in the H → ZZ → 4ℓ decay channel to the standard model expectation, is measured to be μ = 1 05− 0 17+ 0 19 at mH = 125 09 GeV, the combined ATLAS and CMS measurement of the Higgs boson mass