Figure3_LeadJ_X_BH
Figure3 (a)
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Results of applying the BH algorithm to the mass spectra in the leading small-R jet category, using the fitted background...
Figure3 (a)
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Results of applying the BH algorithm to the mass spectra in the leading small-R jet category, using the fitted background...
Figure3 (b)
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Results of applying the BH algorithm to the mass spectra in the leading bjet category, using the fitted background estimations...
Figure3 (c)
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Results of applying the BH algorithm to the mass spectra in the leading large-R jet category, using the fitted background...
Figure3 (d)
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Results of applying the BH algorithm to the mass spectra in the leading photon category, using the fitted background estimations...
Figure3 (e)
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Results of applying the BH algorithm to the mass spectra in the leading electron category, using the fitted background estimations...
Figure3 (f)
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Results of applying the BH algorithm to the mass spectra in the leading muon category, using the fitted background estimations...
Figure4 (a)
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Results of applying the BH algorithm to the mass spectra in the leading small-R jet category, using the fitted background...
Figure4 (b)
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Results of applying the BH algorithm to the mass spectra in the leading bjet category, using the fitted background estimations...
Figure4 (c)
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Results of applying the BH algorithm to the mass spectra in the leading large-R jet category, using the fitted background...
Figure4 (d)
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Results of applying the BH algorithm to the mass spectra in the leading photon category, using the fitted background estimations...
Figure4 (e)
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Results of applying the BH algorithm to the mass spectra in the leading electron category, using the fitted background estimations...
Figure4 (f)
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Results of applying the BH algorithm to the mass spectra in the leading muon category, using the fitted background estimations...
Figure5 (a)
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Results of applying the BH algorithm to the mass spectra in the inclusive category, using the fitted background estimations from...
Figure5 (b)
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Results of applying the BH algorithm to the mass spectra in the inclusive category, using the fitted background estimations from...
Figure6 (a)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure6 (b)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure6 (c)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure6 (d)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure6 (e)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure6 (f)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure7 (a)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure7 (b)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure7 (c)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure7 (d)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure7 (e)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure7 (f)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure8 (a)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure8 (b)
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Upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped signal with a...
Figure9 (a)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure9 (b)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure9 (c)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure9 (d)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure9 (e)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure9 (f)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure10 (a)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure10 (b)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure10 (c)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure10 (d)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure10 (e)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure10 (f)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure11 (a)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure11 (b)
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Comparison of observed upper limits at 95% CL on the cross section times branching fraction times acceptance for a Gaussian-shaped...
Figure12
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Acceptance times efficiency in an HVT model as a function of mass in the leading large-R jet category
Figure13
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Upper limits at 95% CL on the cross section times the branching fraction($W^{\prime} \to ZW$) for the HVT signal as...
Figure14 (a)
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Comparison of the identification efficiencies using standard and merged-ee reconstruction as a function of true PT(Z)
Figure14 (b)
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Background rejection factor as a function of signal efficiency. The red curve shows the BDT performance whereas the blue curve...
Figure15 (a)
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BH p-values of the 100 pseudo-experiments as a function of in the leading small-R jet category for an injected Gaussian-shaped...
Figure15 (b)
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BH p-values of the 100 pseudo-experiments as a function of in the leading small-R jet category for an injected Gaussian-shaped...
Figure16 (a)
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Fractions of pseudo-experiments in which the detected BH interval agrees with the injected mass point and the BH p-value is...
Figure16 (b)
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Fractions of pseudo-experiments in which the detected BH interval agrees with the injected mass point and the BH p-value is...
Figure17 (a)
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Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative...
Figure17 (b)
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Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative...
Figure17 (c)
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Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative...
Figure17 (d)
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Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative...
Figure17 (e)
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Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative...
Figure17 (f)
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Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative...
Table 1
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Data yields of the six event categories in the $Z\to e^+e^-$ and $\mu^+\mu^-$ decay channels. The merged-$e^+e^-$ events are included...
Table 2
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A list of mass spectra, event categories and their corresponding fit ranges, functional forms, numbers of free parameters and global...
Table 3
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A list of mass spectra, event categories and their corresponding signal-sensitive mass ranges. The initial BH $p$-value is obtained by...
Table 4
10.17182/hepdata.132793.v1/t60
A list of mass spectra, event categories, relative width values of Gaussian-shaped signals and limit-sensitive mass ranges and fractions, corresponding...
Table 5
10.17182/hepdata.132793.v1/t61
Cutflow of HVT model $A$ signals ($W^\prime \to ZW \to \ell\ell qq$) with $m_{W^\prime} = 1$ TeV and $m_{W^\prime} =...
Table 6
10.17182/hepdata.132793.v1/t62
Acceptance times efficiency ($\mathcal{A} \times \epsilon$) values in % in the dominant event category for $p^Z_{\mathrm{T}} > 100$ GeV in...
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