2,626 research outputs found

    Resummation Prediction on Higgs and Vector Boson Associated Production with a Jet Veto at the LHC

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    We investigate the resummation effects for the SM Higgs and vector boson associated production at the LHC with a jet veto in soft-collinear effective theory using "collinear anomalous" formalism. We calculate the jet vetoed invariant mass distribution and the cross section for this process at Next-to-Next-to-Leading-Logarithmic level, which are matched to the QCD Next-to-Leading Order results, and compare the differences of the resummation effects with different jet veto pTvetop_{T}^{\rm veto} and jet radius RR. Our results show that both resummation enhancement effects and the scale uncertainties decrease with the increasing of jet veto pTvetop_{T}^{\rm veto} and jet radius RR, respectively. When pTveto=25p_{T}^{\rm veto}=25 GeV and R=0.4 (0.5)R=0.4~(0.5), the resummation effects reduce the scale uncertainties of the Next-to-Leading Order jet vetoed cross sections to about 7% (6%)7\%~(6\%), which lead to increased confidence on the theoretical predictions. Besides, after including resummation effects, the PDF uncertainties of jet vetoed cross section are about 7%7\%.Comment: 22 pages, 10 figures and 2 tables; final version in JHE

    Soft gluon resummation in the signal-background interference process of gg(→h∗)→ZZgg(\to h^*) \to ZZ

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    We present a precise theoretical prediction for the signal-background interference process of gg(→h∗)→ZZgg(\to h^*) \to ZZ, which is useful to constrain the Higgs boson decay width and to measure Higgs couplings to the SM particles. The approximate NNLO KK-factor is in the range of 2.05−2.452.05-2.45 (1.85−2.251.85-2.25), depending on MZZM_{ZZ}, at the 8 (13) TeV LHC. And the soft gluon resummation can increase the approximate NNLO result by about 10%10\% at both the 8 TeV and 13 TeV LHC. The theoretical uncertainties including the scale, uncalculated multi-loop amplitudes of the background and PDF+αs+\alpha_s are roughly O(10%)\mathcal{O}(10\%) at NNLL′{\rm NNLL'}. We also confirm that the approximate KK-factors in the interference and the pure signal processes are the same.Comment: 18 pages, 9 figures; v2 published in JHE
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