Figure 2a
Data from Figure 2 (left)
10.17182/hepdata.166218.v1/t1
Distribution of the invariant mass of the di-$\tau$ system, reconstructed with the FastMTT algorithm, after the full event selection in...
Data from Figure 2 (left)
10.17182/hepdata.166218.v1/t1
Distribution of the invariant mass of the di-$\tau$ system, reconstructed with the FastMTT algorithm, after the full event selection in...
Data from Figure 2 (right)
10.17182/hepdata.166218.v1/t2
Distribution of the invariant mass of the di-$\tau$ system, reconstructed with the FastMTT algorithm, after the full event selection in...
Data from Figure 3 (left)
10.17182/hepdata.166218.v1/t3
Distribution of $M_{\mathrm{H}(\mathrm{b}\bar{\mathrm{b}})}$ obtained from the leading AK8 jet in the event after the full event selection for the $\tau_{\mathrm{h}}\tau_{\mathrm{h}}$...
Data from Figure 3 (right)
10.17182/hepdata.166218.v1/t4
Distribution of $M_{\mathrm{H}(\mathrm{b}\bar{\mathrm{b}})}$ obtained from the leading AK8 jet in the event after the full event selection for the $\ell\tau_{\mathrm{h}}$...
Data from Figure 4 (left)
10.17182/hepdata.166218.v1/t5
Post-fit reconstructed mass distribution of resonance $X$ in the SR after applying all selection criteria, for the sum of the...
Data from Figure 4 (right)
10.17182/hepdata.166218.v1/t6
Post-fit reconstructed mass distribution of resonance $X$ in the SB after applying all selection criteria, for the sum of the...
Data from Figure 5 (left)
10.17182/hepdata.166218.v1/t7
Expected and observed upper limits at 95% CL on the production cross section of resonant HH production for a spin-0...
Data from Figure 5 (right)
10.17182/hepdata.166218.v1/t8
Expected and observed upper limits at 95% CL on the production cross section of resonant HH production for a spin-2...
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