#### ${\mathit {\mathit t}}$-quark EW Couplings

${{\mathit W}}$ helicity fractions in top decays. ${{\mathit F}_{{0}}}$ is the fraction of longitudinal and ${{\mathit F}_{{+}}}$ the fraction of right-handed ${{\mathit W}}$ bosons. ${{\mathit F}_{{{V+A}}}}$ is the fraction of $\mathit V+\mathit A$ current in top decays. The effective Lagrangian (cited by ABAZOV 2008AI) has terms f${}^{L}_{1}$ and f${}^{R}_{1}$ for $\mathit V−\mathit A$ and $\mathit V+\mathit A$ couplings, f${}^{L}_{2}$ and f${}^{R}_{2}$ for tensor couplings with b$_{R}$ and b$_{L}$ respectively.

#### ${\mathit \sigma (}$ ${{\mathit H}}{{\mathit t}}{{\overline{\mathit t}}}{)}$ /${\mathit \sigma (}$ ${{\mathit H}}{{\mathit t}}{{\overline{\mathit t}}}{)}_{SM}$

VALUE CL% DOCUMENT ID TECN  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
$1.43$ ${}^{+0.33}_{-0.31}$ ${}^{+0.21}_{-0.15}$ 1
 2020 Z
ATLS ${{\mathit H}}{{\mathit t}}{{\overline{\mathit t}}}$ ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )
$1.38$ ${}^{+0.29}_{-0.27}$ ${}^{+0.21}_{-0.11}$ 2
 2020 AS
CMS ${{\mathit H}}{{\mathit t}}{{\overline{\mathit t}}}$ ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ )
$0.72$ $\pm0.24$ $\pm0.38$ 3
 2019 R
CMS ${{\mathit H}}{{\mathit t}}{{\overline{\mathit t}}}$ ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit t}}{{\overline{\mathit t}}}$ $\rightarrow$ ${{\mathit \ell}}$ +jets or dilepton)
$0.9$ $\pm0.7$ $\pm1.3$ 4
 2018 BD
CMS ${{\mathit H}}{{\mathit t}}{{\overline{\mathit t}}}$ ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit t}}{{\overline{\mathit t}}}$ $\rightarrow$ all jets)
$1.26$ ${}^{+0.31}_{-0.26}$ 5
 2018 L
CMS combination of CMS
$<6.7$ 95 6
 2015
ATLS ${{\mathit H}}{{\mathit t}}{{\overline{\mathit t}}}$ ; ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$
$2.8$ $\pm1.0$ 7
 2014 H
CMS ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , ${{\mathit \tau}_{{h}}}{{\mathit \tau}_{{h}}}$ , ${{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit W}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit Z}}$ (leptons)
 1 AAD 2020Z based on 139 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at 13 TeV. Assuming a $\mathit CP$-even coupling the ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}}$ process is observed with a significance of 5.2 $\sigma$, and the measured $\sigma _{ {{\mathit t}} {{\overline{\mathit t}}} {{\mathit H}} }\cdot{}\mathit B_{ {{\mathit \gamma}} {{\mathit \gamma}} }$ = $1.64$ ${}^{+0.38}_{-0.36}{}^{+0.17}_{-0.14}$ fb. A $\mathit CP$-mixing angle $\vert \alpha \vert$ $>$ 43$^\circ{}$ is excluded at 95$\%$ CL.
 2 SIRUNYAN 2020AS based on 137 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at 13 TeV. The ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}}$ process is observed with a significance of 6.6 $\sigma$, and the measured $\sigma _{ {{\mathit t}} {{\overline{\mathit t}}} {{\mathit H}} }\cdot{}\mathit B_{ {{\mathit \gamma}} {{\mathit \gamma}} }$ = $1.56$ ${}^{+0.33}_{-0.30}{}^{+0.09}_{-0.08}$ fb. The fractional contribution of the $\mathit CP$-odd component is measured to be f${}^{ {{\mathit t}} {{\overline{\mathit t}}} {{\mathit H}} }_{CP}$ = $0.00$ $\pm0.33$.
 3 SIRUNYAN 2019R based on 35.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at 13 TeV. Multivariate techniques are employed to separate the signal from the dominant ${{\mathit t}}{{\overline{\mathit t}}}$ +jets background. The result is for ${\mathit m}_{{{\mathit H}}}$ = 125 GeV. The measured ratio corresponds to a signal significance of 1.6$\sigma$ above the background-only hypothesis.
 4 SIRUNYAN 2018BD based on 35.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at 13 TeV. A combined fit of signal and background templates to data is performed in six event categories separated by jet and ${{\mathit b}}$ -jet multiplicities. An upper limit of 3.8 is obtained for the cross section ratio.
 5 SIRUNYAN 2018L based on up to 5.1, 19.7, and 35.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at 7, 8, and 13 TeV, respectively. An excess of events is observed, with a significance of 5.2 standard deviations, over the expectation from the background-only hypothesis. The result is for the Higgs boson mass of 125.09 GeV.
 6 Based on 4.5 fb${}^{-1}$ of data at 7 TeV and 20.3 fb${}^{-1}$ at 8 TeV. The result is for ${\mathit m}_{{{\mathit H}}}$ = 125.4 GeV. The measurement constrains the top quark Yukawa coupling strength parameter $\kappa _{t}$ = ${{\mathit Y}_{{t}}}$ /${{\mathit Y}_{{t}}^{SM}}$ to be $-1.3$ $<$ $\kappa _{t}$ $<$ 8.0 (95$\%$ CL).
 7 Based on 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at 7 TeV and 19.7 fb${}^{-1}$ at 8 TeV. The results are obtained by assuming the SM decay branching fractions for the Higgs boson of mass 125.6 GeV. The signal strength for individual Higgs decay channels are given in Fig. 13, and the preferred region in the ($\kappa _{V}$, $\kappa _{f}$) space is given in Fig. 14.
References:
PRL 125 061802 $CP$ Properties of Higgs Boson Interactions with Top Quarks in the $t\bar{t}H$ and $tH$ Processes Using $H \rightarrow \gamma\gamma$ with the ATLAS Detector
PRL 125 061801 Measurements of $\mathrm{t\bar{t}}$H production and the CP structure of the Yukawa interaction between the Higgs boson and top quark in the diphoton decay channel
JHEP 1903 026 Search for $\mathrm{t}\overline{\mathrm{t}}\mathrm{H}$ production in the $\mathrm{H}\to \mathrm{b}\overline{\mathrm{b}}$ decay channel with leptonic $\mathrm{t}\overline{\mathrm{t}}$ decays in proton-proton collisions at $\sqrt{s}=13$ TeV
PRL 120 231801 Observation of $\mathrm{t\overline{t}}$H production
JHEP 1806 101 Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV
PL B740 222 Search for ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ Produced in Association with Top Quarks and Constraints on the Yukawa Coupling between the Top Quark and the Higgs Boson using Data Taken at 7 TeV and 8 TeV with the ATLAS Detector