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Searches for heavy $ZZ$ and $ZW$ resonances in the $\ell\ell qq$ and $\nu\nu qq$ final states in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

The ATLAS collaboration
No Journal Information, 2017

Abstract (data abstract)
CERN-LHC, ATLAS. Acceptance times efficiency Basic event selection: - Additional selection: Signal region (SR): - Control Region (CR): - Validation Region (VR): -

  • Table 1

    Data from Figure 4a

    10.17182/hepdata.78550.v1/t1

    Selection acceptance times efficiency for ggF H -> Z Z -> llqq as a function of the Higgs boson mass,...

  • Table 2

    Data from Figure 4b

    10.17182/hepdata.78550.v1/t2

    Selection acceptance times efficiency for VBF H -> Z Z -> llqq as a function of the Higgs boson mass,...

  • Table 3

    Data from Figure 6a

    10.17182/hepdata.78550.v1/t3

    Selection acceptance times efficiency for ggF H -> Z Z -> vvqq as a function of the Higgs boson mass,...

  • Table 4

    Data from Figure 6b

    10.17182/hepdata.78550.v1/t4

    Selection acceptance times efficiency for VBF H -> ZZ -> vvqq as a function of the Higgs boson mass, combining...

  • Table 5

    Data from Figure 15a

    10.17182/hepdata.78550.v1/t5

    Selection acceptance times efficiency for DY W' -> ZW -> llqq as a function of the W' mass, combining the...

  • Table 6

    Data from Figure 15b

    10.17182/hepdata.78550.v1/t6

    Selection acceptance times efficiency for VBF W' -> ZW -> llqq as a function of the W' mass, combining the...

  • Table 7

    Data from Figure 16a in the auxiliary material

    10.17182/hepdata.78550.v1/t7

    Selection acceptance times efficiency for DY W' -> ZW -> vvqq as a function of the W' mass, combining the...

  • Table 8

    Data from Figure 16b in the auxiliary material

    10.17182/hepdata.78550.v1/t8

    Selection acceptance times efficiency for VBF W' -> ZW -> vvqq as a function of the W' mass, combining the...

  • Table 9

    Data from Figure 17a in the auxiliary material

    10.17182/hepdata.78550.v1/t9

    Selection acceptance times efficiency for G* -> ZZ -> llqq as a function of the W' mass, combining the HP...

  • Table 10

    Data from Figure 17b in the auxiliary material

    10.17182/hepdata.78550.v1/t10

    Selection acceptance times efficiency for G* -> ZZ -> vvqq as a function of the W' mass, combining the HP...

  • Table 11

    Data from Figure 12a

    10.17182/hepdata.78550.v1/t11

    Observed and expected 95% CL upper limits on $\sigma\times$BR($H\to ZZ$) at $\sqrt{s} = 13$ TeV for ggF production of a...

  • Table 12

    Data from Figure 12b

    10.17182/hepdata.78550.v1/t12

    Observed and expected 95% CL upper limits on $\sigma\times$BR($H\to ZZ$) at $\sqrt{s} = 13$ TeV for VBF production of a...

  • Table 13

    Data from Figure 13a

    10.17182/hepdata.78550.v1/t13

    Observed and expected 95% CL upper limits on $\sigma\times$BR($W'\to ZW$) at $\sqrt{s} = 13$ TeV for Drell-Yan production of a...

  • Table 14

    Data from Figure 13b

    10.17182/hepdata.78550.v1/t14

    Observed and expected 95% CL upper limits on $\sigma\times$BR($W'\to ZW$) at $\sqrt{s} = 13$ TeV for VBF production of a...

  • Table 15

    Data from Figure 14a

    10.17182/hepdata.78550.v1/t15

    Observed and expected 95% CL upper limits on $\sigma\times$BR($G_{\mathrm{KK}}\to ZZ$) at $\sqrt{s} = 13$ TeV for the production of a...

  • Table 16

    Data from Figure 14b

    10.17182/hepdata.78550.v1/t16

    Observed and expected 95% CL upper limits on $\sigma\times$BR($G_{\mathrm{KK}}\to ZZ$) at $\sqrt{s} = 13$ TeV for the production of a...

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