| $\bf{
0.320 \pm0.013}$
|
OUR AVERAGE
|
| $> 0.264 \pm0.044$ |
95 |
1 |
|
ATLS |
| $0.323$ $\pm0.008$ $\pm0.014$ |
|
2 |
|
CMS |
| $0.310$ $\pm0.022$ $\pm0.022$ |
|
3 |
|
CMS |
| $0.32$ $\pm0.04$ |
|
4 |
|
ATLS |
|
1
AABOUD 2017BB based on 20.2 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at $\sqrt {s }$ = 8 TeV. Triple-differential decay rate of top quark in the ${{\mathit t}}$-channel single-top production is used to simultaneously determine five generalized ${{\mathit W}}{{\mathit t}}{{\mathit b}}$ couplings as well as the top polarization. No assumption is made for the other couplings. The authors reported ${{\mathit f}_{{1}}}$ = $0.30$ $\pm0.05$ and ${{\mathit f}_{{1}}^{+}}$ $<$ $0.120$ which we converted to ${{\mathit F}_{{-}}}$ = ${{\mathit f}_{{1}}}(1$ $−$ ${{\mathit f}_{{1}}^{+}}$). See this paper for constraints on other couplings not included here.
|
|
2
KHACHATRYAN 2016BU based on 19.8 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at $\sqrt {s }$ = 8 TeV using ${{\mathit t}}{{\overline{\mathit t}}}$ events with ${{\mathit \ell}}$ + $\not E_T$ + ${}\geq{}$4 jets(${}\geq{}$2 ${{\mathit b}}$). The errors of ${{\mathit F}_{{0}}}$ and ${{\mathit F}_{{-}}}$ are correlated with a correlation coefficient $\rho ({{\mathit F}_{{0}}}$, ${{\mathit F}_{{-}}}$) = $-0.87$. The result is consistent with the NNLO SM prediction of $0.311$ $\pm0.005$ for ${\mathit m}_{{{\mathit t}}}$ = $172.8$ $\pm1.3$ GeV.
|
|
3
Based on 5.0 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at $\sqrt {s }$ = 7 TeV. CHATRCHYAN 2013BH studied events with large $\not E_T$ and ${{\mathit \ell}}$ +${}\geq{}$4 jets using a constrained kinematic fit.
|
|
4
Based on 1.04 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at $\sqrt {s }$ = 7 TeV. AAD 2012BG studied events with large $\not E_T$ and either ${{\mathit \ell}}$ +${}\geq{}$4j or ${{\mathit \ell}}{{\mathit \ell}}$ +${}\geq{}$2j. The uncertainties are not independent, $\rho ({{\mathit F}_{{0}}},{{\mathit F}_{{-}}}$) = $-0.96$.
|
