Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at √s=13 TeV

dc.contributor.author Sirunyan, A. M.
dc.contributor.author Tumasyan, A.
dc.contributor.author Adam, W.
dc.contributor.author Ambrogi, F.
dc.contributor.author Asilar, E.
dc.contributor.author Bergauer, T.
dc.contributor.author Brandstetter, J.
dc.contributor.author Brondolin, E.
dc.contributor.author Dragicevic, M.
dc.contributor.author Erö, J.
dc.contributor.author Flechl, M.
dc.contributor.author Friedl, M.
dc.contributor.author Frühwirth, R.
dc.contributor.author Ghete, V. M.
dc.contributor.author Grossmann, J.
dc.contributor.author Hrubec, J.
dc.contributor.author Jeitler, M.
dc.contributor.author König, A.
dc.contributor.author Krammer, N.
dc.contributor.author Krätschmer, I.
dc.contributor.author Liko, D.
dc.contributor.author Madlener, T.
dc.contributor.author Mikulec, I.
dc.contributor.author Pree, E.
dc.contributor.author Rabady, D.
dc.contributor.author Rad, N.
dc.contributor.author Rohringer, H.
dc.contributor.author Schieck, J.
dc.contributor.author Schöfbeck, R.
dc.contributor.author Spanring, M.
dc.contributor.author Spitzbart, D.
dc.contributor.author Waltenberger, W.
dc.contributor.author Wittmann, J.
dc.contributor.author Wulz, C. E.
dc.contributor.author Zarucki, M.
dc.contributor.author Chekhovsky, V.
dc.contributor.author Mossolov, V.
dc.contributor.author Suarez Gonzalez, J.
dc.contributor.author De Wolf, E. A.
dc.contributor.author Di Croce, D.
dc.contributor.author Janssen, X.
dc.contributor.author Lauwers, J.
dc.contributor.author Van Haevermaet, H.
dc.contributor.author Van Mechelen, P.
dc.contributor.author Van Remortel, N.
dc.contributor.author Abu Zeid, S.
dc.contributor.author Blekman, F.
dc.contributor.author D’Hondt, J.
dc.contributor.author De Bruyn, I.
dc.contributor.author De Clercq, J.
dc.contributor.author Deroover, K.
dc.contributor.author Flouris, G.
dc.contributor.author Lontkovskyi, D.
dc.contributor.author Lowette, S.
dc.contributor.author Moortgat, S.
dc.contributor.author Moreels, L.
dc.contributor.author Olbrechts, A.
dc.contributor.author Python, Q.
dc.contributor.author Skovpen, K.
dc.contributor.author Tavernier, S.
dc.contributor.author Van Doninck, W.
dc.contributor.author Van Mulders, P.
dc.contributor.author Van Parijs, I.
dc.contributor.author Brun, H.
dc.contributor.author Clerbaux, B.
dc.contributor.author De Lentdecker, G.
dc.contributor.author Delannoy, H.
dc.contributor.author Fasanella, G.
dc.contributor.author Favart, L.
dc.contributor.author Goldouzian, R.
dc.contributor.author Grebenyuk, A.
dc.contributor.author Karapostoli, G.
dc.contributor.author Lenzi, T.
dc.contributor.author Luetic, J.
dc.contributor.author Maerschalk, T.
dc.contributor.author Marinov, A.
dc.contributor.author Randle-conde, A.
dc.contributor.author Seva, T.
dc.contributor.author Vander Velde, C.
dc.contributor.author Vanlaer, P.
dc.contributor.author Vannerom, D.
dc.contributor.author Yonamine, R.
dc.contributor.author Zenoni, F.
dc.contributor.author Zhang, F.
dc.contributor.author Cimmino, A.
dc.contributor.author Cornelis, T.
dc.contributor.author Dobur, D.
dc.contributor.author Fagot, A.
dc.contributor.author Gul, M.
dc.contributor.author Khvastunov, I.
dc.contributor.author Poyraz, D.
dc.contributor.author Roskas, C.
dc.contributor.author Salva, S.
dc.contributor.author Tytgat, M.
dc.contributor.author Verbeke, W.
dc.contributor.author Zaganidis, N.
dc.contributor.author Bakhshiansohi, H.
dc.contributor.author Bondu, O.
dc.contributor.author Brochet, S.
dc.date.accessioned 2022-03-27T06:51:31Z
dc.date.available 2022-03-27T06:51:31Z
dc.date.issued 2017-11-01
dc.description.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. 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. The signal strength modifiers for the individual Higgs boson production modes are also measured. The cross section in the fiducial phase space defined by the requirements on lepton kinematics and event topology is measured to be 2. 92− 0.44+ 0.48(stat)− 0.24+ 0.28(syst)fb, which is compatible with the standard model prediction of 2.76 ± 0.14 fb. Differential cross sections are reported as a function of the transverse momentum of the Higgs boson, the number of associated jets, and the transverse momentum of the leading associated jet. The Higgs boson mass is measured to be mH = 125.26 ± 0.21 GeV and the width is constrained using the on-shell invariant mass distribution to be ΓH < 1.10 GeV, at 95% confidence level.[Figure not available: see fulltext.]
dc.identifier.citation Journal of High Energy Physics. v.2017(11)
dc.identifier.issn 11266708
dc.identifier.uri 10.1007/JHEP11(2017)047
dc.identifier.uri https://link.springer.com/10.1007/JHEP11(2017)047
dc.identifier.uri https://dspace.uohyd.ac.in/handle/1/10398
dc.subject Hadron-Hadron scattering (experiments)
dc.subject Higgs physics
dc.title Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at √s=13 TeV
dc.type Journal. Article
dspace.entity.type
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