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Title: Constraints on new phenomena via Higgs boson couplings and invisible decays with the ATLAS detector
Authors: Hrynevich, A.
ATLAS Collaboration
Keywords: ЭБ БГУ::ЕСТЕСТВЕННЫЕ И ТОЧНЫЕ НАУКИ::Физика
ЭБ БГУ::ТЕХНИЧЕСКИЕ И ПРИКЛАДНЫЕ НАУКИ. ОТРАСЛИ ЭКОНОМИКИ::Ядерная техника
Issue Date: 2015
Publisher: Springer Verlag
Citation: J High Energy Phys 2015;2015(11):1-52.
Abstract: The ATLAS experiment at the LHC has measured the Higgs boson couplings and mass, and searched for invisible Higgs boson decays, using multiple production and decay channels with up to 4.7 fb−1 of pp collision data at−1at TeV. In the current study, the measured production and decay rates of the observed Higgs boson in the γγ, ZZ, W W , Zγ, bb, τ τ , and μμ decay channels, along with results from the associated production of a Higgs boson with a top-quark pair, are used to probe the scaling of the couplings with mass. Limits are set on parameters in extensions of the Standard Model including a composite Higgs boson, an additional electroweak singlet, and two-Higgs-doublet models. Together with the measured mass of the scalar Higgs boson in the γγ and ZZ decay modes, a lower limit is set on the pseudoscalar Higgs boson mass of mA> 370 GeV in the “hMSSM” simplified Minimal Supersymmetric Standard Model. Results from direct searches for heavy Higgs bosons are also interpreted in the hMSSM. Direct searches for invisible Higgs boson decays in the vector-boson fusion and associated production of a Higgs boson with W/Z (Z → ℓℓ, W/Z → jj) modes are statistically combined to set an upper limit on the Higgs boson invisible branching ratio of 0.25. The use of the measured visible decay rates in a more general coupling fit improves the upper limit to 0.23, constraining a Higgs portal model of dark matter
URI: https://elib.bsu.by/handle/123456789/264661
DOI: 10.1007/JHEP11(2015)206
Scopus: 84949684350
Sponsorship: ST/N000420/1; National Science Foundation,1119200,1506173; Seventh Framework Programme ( FP7), 246806; Science and Technology Facilities Council Посмотреть возможности по STFC PP/D002915/1,PP/E000347/1,PP/E000355/1,PP/E000444/1,PP/E002846/1,PP/E003087/1,ST/G50228X/1,ST/G502320/1,ST/H00100X/1,ST/H00100X/2,ST/H001093/1,ST/H001093/2,ST/I000178/1,ST/I000186/1,ST/I00372X/1,ST/I005803/1,ST/I006056/1,ST/I006080/1,ST/J00474X/1,ST/J004928/1,ST/J004944/1,ST/J005487/1,ST/J005525/1,ST/J005576/1,ST/K000705/1,ST/K00073X/1,ST/K001248/1,ST/K001302/1,ST/K001310/1,ST/K001329/1,ST/K001361/1,ST/K00137X/1,ST/K00140X/1,ST/K001418/1,ST/K003658/1,ST/L000326/1,ST/L000970/1,ST/L001144/1,ST/L001179/1,ST/L001195/1,ST/L003112/1,ST/L003325/1,ST/L003414/1,ST/L003511/1,ST/L00352X/1,ST/L006464/1,ST/L006480/1,ST/M000761/1,ST/M001407/1,ST/M001431/1,ST/M001474/1,ST/M001504/1,ST/M001733/1,ST/M002306/1,ST/M003213/1,ST/M004821/1,ST/M006980/1,ST/N000277/1,ST/N000307/1,ST/N000463/1 STFC Japan Society for the Promotion of Science Посмотреть возможности по JSPS 26247040 JSPS Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung (SFN), PP/D002915/1,PP/E000347/1,PP/E000355/1,PP/E000444/1,PP/E002846/1,PP/E003087/1,ST/G50228X/1,ST/G502320/1,ST/H00100X/1,ST/H00100X/2,ST/H001093/1,ST/H001093/2,ST/I000178/1,ST/I000186/1,ST/I00372X/1,ST/I005803/1,ST/I006056/1,ST/I006080/1,ST/J00474X/1,ST/J004928/1,ST/J004944/1,ST/J005487/1,ST/J005525/1,ST/J005576/1,ST/K000705/1,ST/K00073X/1,ST/K001248/1,ST/K001302/1,ST/K001310/1,ST/K001329/1,ST/K001361/1,ST/K00137X/1,ST/K00140X/1,ST/K001418/1,ST/K003658/1,ST/L000326/1,ST/L000970/1,ST/L001144/1,ST/L001179/1,ST/L001195/1,ST/L003112/1,ST/L003325/1,ST/L003414/1,ST/L003511/1,ST/L00352X/1,ST/L006464/1,ST/L006480/1,ST/M000761/1,ST/M001407/1,ST/M001431/1,ST/M001474/1,ST/M001504/1,ST/M001733/1,ST/M002306/1,ST/M003213/1,ST/M004821/1,ST/M006980/1,ST/Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung 156083N000277/1,ST/N000307/1,ST/N000463/1; Japan Society for the Promotion of Science ( JSPS),26247040;
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