Measurement of the Higgs boson production rate in association with top quarks in final states with electrons, muons, and hadronically decaying tau leptons at $\sqrt{s} =$ 13 TeV

The collaboration
Eur.Phys.J.C 81 (2021) 378, 2021.

Abstract
The rate for Higgs (H) bosons production in association with either one (tH) or two ($\mathrm{t\bar{t}}$H) top quarks is measured in final states containing multiple electrons, muons, or tau leptons decaying to hadrons and a neutrino, using proton-proton collisions recorded at a center-of-mass energy of 13 TeV by the CMS experiment. The analyzed data correspond to an integrated luminosity of 137 fb$^{-1}$. The analysis is aimed at events that contain H $\to$ WW, H $\to$$\tau\tau, or H \to ZZ decays and each of the top quark(s) decays either to lepton+jets or all-jet channels. Sensitivity to signal is maximized by including ten signatures in the analysis, depending on the lepton multiplicity. The separation among the tH, the \mathrm{t\bar{t}}H, and the backgrounds is enhanced through machine-learning techniques and matrix-element methods. The measured production rates for the \mathrm{t\bar{t}}H and tH signals correspond to 0.92 \pm 0.19 (stat) ^{+0.17}_{-0.13} (syst) and 5.7 \pm 2.7 (stat) \pm 3.0 (syst) of their respective standard model (SM) expectations. The corresponding observed (expected) significance amounts to 4.7 (5.2) standard deviations for \mathrm{t\bar{t}}H, and to 1.4 (0.3) for tH production. Assuming that the Higgs boson coupling to the tau lepton is equal in strength to its expectation in the SM, the coupling y_{\mathrm{t}} of the Higgs boson to the top quark divided by its SM expectation, \kappa_\mathrm{t} = y_\mathrm{t} / y_\mathrm{t}^\mathrm{SM}, is constrained to be within -0.9 \lt$$\kappa_\mathrm{t}$$\lt$$-$0.7 or 0.7 $\lt$$\kappa_\mathrm{t}$$\lt$ 1.1, at 95% confidence level. This result is the most sensitive measurement of the $\mathrm{t\bar{t}}$H production rate to date.

• #### Table 6

Table 6

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Number of events selected in the $3\ell$- and $4\ell$-CRs and in the CR for the ttW background, compared to the...

• #### Table 7

Table 7

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Summary of the sources of systematic and statistical uncertainties and their impact on the measurement of the ttH and tH...

• #### Table 8 1

Table 8

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Number of events selected in the 2$\ell$ss+0$\tau_{\mathrm{h}}$, 3$\ell$+0$\tau_{\mathrm{h}}$, and 2$\ell$ss+1$\tau_{\mathrm{h}}$ analysis channels compared to the event yields expected from the...

• #### Table 8 2

Table 8

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Number of events selected in the 1$\ell$+1$\tau_{\mathrm{h}}$, 0$\ell$+2$\tau_{\mathrm{h}}$, 2$\ell$os+1$\tau_{\mathrm{h}}$, and 1$\ell$+2$\tau_{\mathrm{h}}$ analysis channels compared to the event yields expected from...

• #### Table 8 3

Table 8

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Number of events selected in the 4$\ell$+0$\tau_{\mathrm{h}}$, 3$\ell$+1$\tau_{\mathrm{h}}$, and 2$\ell$+2$\tau_{\mathrm{h}}$ analysis channels compared to the event yields expected from the...

• #### Figure 17

Figure 17

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Dependence of the likelihood function L as a function of $\kappa_{\mathrm{t}}$ and $\kappa_{\mathrm{V}}$.

• #### Figure 15 - ttH tH

Figure 15

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$-2\Delta log( L)$ as a function of the production rate of ttH and tH.

• #### Figure 15 - ttH ttW

Figure 15

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$-2\Delta log( L)$ as a function of the production rate of ttH and ttW.

• #### Figure 15 - ttH ttZ

Figure 15

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$-2\Delta log( L)$ as a function of the production rate of ttH and ttZ.

• #### Figure 15 - ttW ttZ

Figure 15

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$-2\Delta log( L)$ as a function of the production rate of ttW and ttZ.

• #### Covariance matrix

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Covariance matrix of the fitted parameters of interest.

• #### Figure 14 (ttH)

Figure 14

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Production rate of the ttH signal measured in each of the ten channels individually and for the combination of all...

• #### Figure 14 (tH)

Figure 14

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Production rate of the tH signal measured in each of the ten channels individually and for the combination of all...

• #### ttH acceptance

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Probability for ttH signal events to pass the event selection in each of the analysis categories employed.

Version 2 modifications: Contents are approved