#### ${\mathit {\mathit t}}$-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.

#### ${{\mathit t}}$ -Quark Yukawa Coupling from ${{\mathit t}}{{\overline{\mathit t}}}$ Kinematic Distributions in ${{\mathit p}}{{\mathit p}}$ Collisions

The ratio of ${{\mathit t}}$ -quark Yukawa coupling to its standard model predicted value.
VALUE DOCUMENT ID TECN  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
$1.16$ ${}^{+0.24}_{-0.35}$ 1
 2020 BH
CMS ${{\mathit \ell}}{{\mathit \ell}}$ (${{\mathit \ell}}$ =${{\mathit e}}$ ,${{\mathit \mu}}$ ) + jets (${}\geq{}2{{\mathit b}}$ j) + $\not E_T$
$1.07$ ${}^{+0.34}_{-0.43}$ 2
 2019 BY
CMS ${{\mathit \ell}}$ +jets, ${{\mathit t}}{{\overline{\mathit t}}}$ threshold
 1 SIRUNYAN 2020BH based on 137 ${\mathrm {fb}}{}^{-1}$ of data at $\sqrt {s }$ = 13 TeV. Kinematic distributions of ${{\mathit t}}{{\overline{\mathit t}}}$ are compared with predictions by different values of the top Yukawa coupling in loop corrections, where the scaling of the SM coupling is used within the $\kappa$-framework. The $\not E_T$ cut applies only to the same-flavor dilepton, not ${{\mathit e}}{{\mathit \mu}}$ events.
 2 SIRUNYAN 2019BY based on 35.8 ${\mathrm {fb}}{}^{-1}$ of data at $\sqrt {s }$ = 13 TeV. Experimental sensitivity is enhanced in the low $\mathit M_{ {{\mathit t}} {{\overline{\mathit t}}} }$ region. The distributions of $\mathit M_{ {{\mathit t}} {{\overline{\mathit t}}} }$, $\vert \mathit y_{t}$ $−$ $\mathit y_{{{\overline{\mathit t}}} }\vert$, and the number of reconstructed jets are compared with predictions by different Yukawa couplings which include NNLO QCD and NLO EW corrections.
References:
 SIRUNYAN 2020BH
PR D102 092013 Measurement of the top quark Yukawa coupling from $\mathrm{t\bar{t}}$ kinematic distributions in the dilepton final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV
 SIRUNYAN 2019BY
PR D100 072007 Measurement of the top quark Yukawa coupling from $\mathrm{t\bar{t}}$ kinematic distributions in the lepton+jets final state in proton-proton collisions at $\sqrt{s} =$ 13 TeV