Table 11.

Observed imits on $(f_{g2},{\mathit{\varphi }}_{g2})$ and $(f_{g4},{\mathit{\varphi }}_{g4})$ parameters defined in Ref. [3] obtained in the analyses of the $H\to W{W}^{\ast }\to e\mathit{\nu }\mathit{\mu }\mathit{\nu }$ and $H\to Z{Z}^{\ast }\to 4\ell$ channels and for their combination

Observed 95 % CL limits
$H\to W{W}^{\ast }\to e\mathit{\nu }\mathit{\mu }\mathit{\nu }$
$f_{g2}<0.053$ for ${\mathit{\varphi }}_{g2}=0$ and $f_{g2}<0.20;0.26<f_{g2}<0.63$ for ${\mathit{\varphi }}_{g2}=\mathit{\pi }$
$f_{g4}<0.78$ for ${\mathit{\varphi }}_{g4}=0$ and $f_{g4}<0.84$ for ${\mathit{\varphi }}_{g4}=\mathit{\pi }$
$H\to Z{Z}^{\ast }\to 4\ell$
$f_{g2}<0.68$ for ${\mathit{\varphi }}_{g2}=0$ and $f_{g2}<0.16$ for ${\mathit{\varphi }}_{g2}=\mathit{\pi }$
$f_{g4}<0.11$ for ${\mathit{\varphi }}_{g4}=0$ and $f_{g4}<0.54$ for ${\mathit{\varphi }}_{g4}=\mathit{\pi }$
Combination of $H\to Z{Z}^{\ast }\to 4\ell$ and $H\to W{W}^{\ast }\to e\mathit{\nu }\mathit{\mu }\mathit{\nu }$
$f_{g2}<0.12$ for ${\mathit{\varphi }}_{g2}=0$ and $f_{g2}<0.16$ for ${\mathit{\varphi }}_{g2}=\mathit{\pi }$
$f_{g4}<0.090$ for ${\mathit{\varphi }}_{g4}=0$ and $f_{g4}<0.41$ for ${\mathit{\varphi }}_{g4}=\mathit{\pi }$