Abstract (data abstract)

CERN-LHC. Search for heavy ZZ resonances in the 4l and 2l2nu final states using proton-proton collisions at a center-of-mass energy of 13 TeV with 139 fb^{-1} of data collected from 2015 to 2018 with the ATLAS detector. Different mass ranges for the hypothetical resonances are considered, depending on the final state and model. The different ranges span between 200 GeV and 2000 GeV. The results are interpreted as upper limits on the production cross section of a spin-0 or spin-2 resonance.

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Figure 2(a) from page 23 of preprint (arxiv)

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Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-high 4-muon category.
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Figure 2(b) from page 23 of preprint (arxiv)

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Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-high 2e2mu category.
Table 3

Figure 2(c) from page 23 of preprint (arxiv)

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Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-high 4-electron category.
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Figure 2(d) from page 23 of preprint (arxiv)

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Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-low category.
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Figure 2(e) from page 23 of preprint (arxiv)

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Distribution of the four-lepton invariant mass in the four-lepton final state for the VBF-MVA-enriched category.
Table 6

Figure 3(a) from page 24 of preprint (arxiv)

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Distribution of the transverse mass in the llvv final state for the ggF-enriched eevv category.
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Figure 3(b) from page 24 of preprint (arxiv)

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Distribution of the transverse mass in the llvv final state for the ggF-enriched mumuvv category.
Table 8

Figure 3(c) from page 24 of preprint (arxiv)

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Distribution of the transverse mass in the llvv final state for the VBF-enriched eevv category.
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Figure 3(d) from page 24 of preprint (arxiv)

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Distribution of the transverse mass in the llvv final state for the VBF-enriched mumuvv category.
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Figure 4(a) from page 25 of preprint (arxiv)

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The upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance...
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Figure 4(b) from page 25 of preprint (arxiv)

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The upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance...
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Figure 5(a) from page 26 of preprint (arxiv)

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The upper limits at 95% CL on the cross section for the ggF production mode times branching ratio as a...
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Figure 5(b) from page 25 of preprint (arxiv)

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The upper limits at 95% CL on the cross section for the ggF production mode times branching ratio as a...
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Figure 5(c) from page 25 of preprint (arxiv)

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The upper limits at 95% CL on the cross section for the ggF production mode times branching ratio as a...
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Figure 5(d) from page 25 of preprint (arxiv)

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The upper limits at 95% CL on the cross section for the ggF production mode times branching ratio as a...
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Figure 8 from page 29 of preprint (arxiv)

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The upper limits at 95% CL on the cross section times branching ratio for a KK graviton produced with k/M_{PI}...

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