2017
DOI: 10.1007/jhep11(2017)047
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Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at $$ \sqrt{s}=13 $$ TeV

Abstract: Properties of the Higgs boson are measured in the H → ZZ → 4 ( = 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. The signal strength modifier µ, defined as the ratio of the observed Higgs boson rate in the H → ZZ → 4 decay channel to the standard model expectation, is measured to be µ = 1.05 +0.19−0.17 at m H = 125.09 GeV, the combined ATLAS and CMS measurement of the … Show more

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Cited by 189 publications
(177 citation statements)
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“…Besides, we use the framework implemented in HIGGSSIGNALS-2 [86] to perform a Higgs data fitting. Experimental data from 7 þ 8 TeV ATLAS and CMS combined Higgs measurements [87] and two 13 TeV Higgs measurements with a higher precision [88,89] are included in the fit. The Higgs signal strength is required to lie within 2σ C.L.…”
Section: B Collider Direct Search and Higgs Datamentioning
confidence: 99%
“…Besides, we use the framework implemented in HIGGSSIGNALS-2 [86] to perform a Higgs data fitting. Experimental data from 7 þ 8 TeV ATLAS and CMS combined Higgs measurements [87] and two 13 TeV Higgs measurements with a higher precision [88,89] are included in the fit. The Higgs signal strength is required to lie within 2σ C.L.…”
Section: B Collider Direct Search and Higgs Datamentioning
confidence: 99%
“…It started at LEP, continued at the Tevatron and culminated in 2012 with the discovery of a spin-0 resonance h with a mass of around 125 GeV at the LHC. In the last five years the LHC Higgs program has matured [1], providing precise measurements of processes such as pp → h → γγ and pp → h → ZZ * → 4 (for the latest LHC results at √ s = 13 TeV see [2][3][4][5]) with SM rates of order 0.1 pb and below. Although the 125 GeV spin-0 resonance has properties very close to the one expected for the SM Higgs, it is still well possible that a non-minimal Higgs sector is realised in nature while h is SM-like.…”
Section: Introductionmentioning
confidence: 99%
“…This makes the CDF four photon search insensitive to custodial fermiophobic Higgs bosons. 6 As emphasized in [15], diphoton searches have the advantage that, being more inclusive, are more model independent and can be applied even in the custodial limit of degenerate masses as well as when M H ± < M H 0 or if the charged Higgs decays in a way that is difficult to observe. Combining updated 8 and 13 TeV low mass diphoton data [37,38], we can obtain new robust bounds on the allowed branching ratio into photons for different cases of custodial fermiophobic Higgs bosons in the mass range 65 − 160 GeV.…”
Section: Lhc Diphoton Limits and 95 Gev Excessmentioning
confidence: 99%
“…In this case branching ratios up to ∼ 5 − 10% are still allowed at low masses while at high masses they can be as large as ∼ 30%. 6 Of course if there are additional Higgs scalars which are in different custodial representations than H 0 F , additional Higgs pair production mechanisms with non-degenerate masses can become available allowing for 4γ + X limits to again be applied.…”
Section: Lhc Diphoton Limits and 95 Gev Excessmentioning
confidence: 99%