handle: 11104/0364435
The CP properties of the coupling between the Higgs boson and the top quark are investigated using 139 fb−1 of proton–proton collision data recorded by the ATLAS experiment at the LHCat a centre-of-mass energy of √s = 13 TeV. The CP structure of the top quark–Higgs boson Yukawa coupling is probed in events with a Higgs boson decaying into a pair of b-quarks and produced in association with either a pair of top quarks, t- th, or a single top quark, th Events containing one or two electrons or muons are used for the measurement. Multivariate techniques are used to select regions enriched in t- tH and tH events, where dedicated CP-sensitive observables are exploited. In an extension of the Standard Model (SM) with a CP-odd admixture in the top–Higgs Yukawa coupling, the mixing angle between CP-even and CP-odd couplings is measured to be α = 11◦+52◦−73◦ , compatible with the SM prediction corresponding to α = 0.
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handle: 11104/0364435
The CP properties of the coupling between the Higgs boson and the top quark are investigated using 139 fb−1 of proton–proton collision data recorded by the ATLAS experiment at the LHCat a centre-of-mass energy of √s = 13 TeV. The CP structure of the top quark–Higgs boson Yukawa coupling is probed in events with a Higgs boson decaying into a pair of b-quarks and produced in association with either a pair of top quarks, t- th, or a single top quark, th Events containing one or two electrons or muons are used for the measurement. Multivariate techniques are used to select regions enriched in t- tH and tH events, where dedicated CP-sensitive observables are exploited. In an extension of the Standard Model (SM) with a CP-odd admixture in the top–Higgs Yukawa coupling, the mixing angle between CP-even and CP-odd couplings is measured to be α = 11◦+52◦−73◦ , compatible with the SM prediction corresponding to α = 0.
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citations | 0 | |
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impulse | Average |
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