Table 6.

Expected and observed p-values for different spin-parity hypotheses, for the combination of the three channels: $H\to \mathit{\gamma }\mathit{\gamma }$ , $H\to Z{Z}^{\ast }\to 4\ell$ and $H\to W{W}^{\ast }\to e\mathit{\nu }\mathit{\mu }\mathit{\nu }$. The observed ${\mathrm{CL}}_{\mathrm{s}}$ for the alternative hypothesis is reported in the last column. The expected and observed p-values and the observed ${\mathrm{CL}}_{\mathrm{s}}$ are defined in Sect. 5.5. The definitions of alternative hypotheses are given in Sect. 3

Tested hypothesis	$p_{\exp ,\mathit{\mu }=1}^{\mathrm{alt}}$	$p_{\exp ,\mathit{\mu }=\widehat{\mathit{\mu }}}^{\mathrm{alt}}$	$p_{\mathrm{obs}}^{\mathrm{SM}}$	$p_{\mathrm{obs}}^{\mathrm{alt}}$	Obs. ${\mathrm{CL}}_{\mathrm{s}}$ (%)
$0_h^{+}$	$2.5\times {10}^{-2}$	$4.7\times {10}^{-3}$	0.85	$7.1\times {10}^{-5}$	$4.7\times {10}^{-2}$
$0^{-}$	$1.8\times {10}^{-3}$	$1.3\times {10}^{-4}$	0.88	$<3.1\times {10}^{-5}$	$<2.6\times {10}^{-2}$
$2^{+}({\mathit{\kappa }}_q={\mathit{\kappa }}_g)$	$4.3\times {10}^{-3}$	$2.9\times {10}^{-4}$	0.61	$4.3\times {10}^{-5}$	$1.1\times {10}^{-2}$
$2^{+}({\mathit{\kappa }}_q=0;p_{\text{T}}<300\text{GeV})$	$<3.1\times {10}^{-5}$	$<3.1\times {10}^{-5}$	0.52	$<3.1\times {10}^{-5}$	$<6.5\times {10}^{-3}$
$2^{+}({\mathit{\kappa }}_q=0;p_{\text{T}}<125\text{GeV})$	$3.4\times {10}^{-3}$	$3.9\times {10}^{-4}$	0.71	$4.3\times {10}^{-5}$	$1.5\times {10}^{-2}$
$2^{+}({\mathit{\kappa }}_q=2{\mathit{\kappa }}_g;p_{\text{T}}<300\text{GeV})$	$<3.1\times {10}^{-5}$	$<3.1\times {10}^{-5}$	0.28	$<3.1\times {10}^{-5}$	$<4.3\times {10}^{-3}$
$2^{+}({\mathit{\kappa }}_q=2{\mathit{\kappa }}_g;p_{\text{T}}<125\text{GeV})$	$7.8\times {10}^{-3}$	$1.2\times {10}^{-3}$	0.80	$7.3\times {10}^{-5}$	$3.7\times {10}^{-2}$