ATLAS
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Constraints on Higgs boson properties using WW(eνμν)jjWW^{*}(\rightarrow e\nu \mu \nu )jj production in 36.1\,\mathrm{fb}^{-1} of s=13\sqrt{s}=13 TeV pp collisions with the ATLAS detector

This article presents the results of two studies of Higgs boson properties using the WW(eνμν)jjWW^*(\rightarrow e\nu\mu\nu)jj final state, based on a dataset corresponding to 36.1 fb1^{-1} of s=13\sqrt{s}=13 TeV proton-proton collisions recorded by the ATLAS experiment at the Large Hadron Collider. The first study targets Higgs boson production via gluon-gluon fusion and constrains the CP properties of the effective Higgs-gluon interaction. Using angular distributions and the overall rate, a value of tan(α)=0.0±0.4(stat.)±0.3(syst.)\tan(\alpha) = 0.0 \pm 0.4 (\mathrm{stat.}) \pm 0.3 (\mathrm{syst.}) is obtained for the tangent of the mixing angle for CP-even and CP-odd contributions. The second study exploits the vector-boson fusion production mechanism to probe the Higgs boson couplings to longitudinally and transversely polarised WW and ZZ bosons in both the production and the decay of the Higgs boson; these couplings have not been directly constrained previously. The polarisation-dependent coupling-strength scale factors are defined as the ratios of the measured polarisation-dependent coupling strengths to those predicted by the Standard Model, and are determined using rate and kinematic information to be aL=0.910.18+0.10a_\mathrm{L}=0.91^{+0.10}_{-0.18}(stat.)0.17+0.09^{+0.09}_{-0.17}(syst.) and aT=1.2±0.4a_{\mathrm{T}}=1.2 \pm 0.4 (stat.)0.3+0.2 ^{+0.2}_{-0.3} (syst.). These coupling strengths are translated into pseudo-observables, resulting in κVV=0.910.18+0.10\kappa_{VV}= 0.91^{+0.10}_{-0.18}(stat.)0.17+0.09^{+0.09}_{-0.17}(syst.) and ϵVV=0.130.20+0.28\epsilon_{VV} =0.13^{+0.28}_{-0.20} (stat.)0.10+0.08^{+0.08}_{-0.10}(syst.). All results are consistent with the Standard Model predictions.

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