ZZ production at hadron colliders in NNLO QCD

Abstract

We report on the first calculation of next-to-next-to-leading order (NNLO) QCD corrections to the inclusive production of ZZ pairs at hadron colliders. Numerical results are presented for pp collisions with centre-of-mass energy ($\sqrt{s}$) ranging from 7 to 14 TeV. The NNLO corrections increase the NLO result by an amount varying from $11\%$ to $17\%$ as $\sqrt{s}$ goes from 7 to 14 TeV. The loop-induced gluon fusion contribution provides about $60\%$ of the total NNLO effect. When going from NLO to NNLO the scale uncertainties do not decrease and remain at the $\pm 3\%$ level.

arXiv commentReference added, version published on Physics Letters B

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• Theory Summary and Prospects
• Higgs couplings in SMEFT via Zh production at the HL-LHC
• NLO EW and QCD corrections to polarized ZZ production in the four-charged-lepton channel at the LHC
• The Beautiful Physics of LHC Run 2
• Hard processes in multi-TeV ion collisions
• A method for correcting the substructure of multiprong jets using the Lund jet plane
• Polarisation at NLO in WZ production at the LHC
• Threshold resummation for $Z$-boson pair production at NNLO+NNLL
• Measurements of $W^{+}{W}^{-}$ production cross-sections in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
• Triply charged Higgs bosons at a 100 TeV $pp$ collider
• QCD and High Energy Interactions: Moriond 2014 Theory Summary
• Measurement of the inclusive and differential $\mathrm{t}\overline{\mathrm{t}}\gamma$ cross sections in the single-lepton channel and EFT interpretation at $\sqrt{s}$ = 13 TeV
• Search for dark matter production in association with a single top quark in proton-proton collisions at $\sqrt{s}$ = 13 TeV
• Di-vector Boson Production with Jets at the LHC
• Higher-Order Corrections to Higgs Boson Amplitudes with Full Quark Mass Dependence in Quantum Chromodynamics
• Improving the Direct Determination of $|V_{ts}|$ using Deep Learning
• QCD Beyond Leading Power
• Probing the flavour structure of dimension-6 EFT operators in multilepton final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV
• SUSY at the LHC without Missing P_T
• NLO QCD corrections to the processes pp $\to$ ZZ with 0, 1 and 2 jets at the LHC