Table 10.

The measured differential fiducial cross section and $\pm 1$ standard deviation uncertainties for the $p_{\mathrm{T}}^{\mathrm{H}}$ observable at $m_{\mathrm{H}}=125.38\text{GeV}$. The breakdown of the total uncertainty (unc.) into statistical and systematic components is given

Bin range ($\text{GeV}$)	$\text{d}{\sigma }_{\mathrm{fid}}$ (fb)	unc.	$\text{(stat)}$	$\text{(syst)}$
0–10	0.32	${}_{-0.10}^{+0.11}$	${}_{-0.09}^{+0.10}$	${}_{-0.03}^{+0.04}$
10–20	0.67	${}_{-0.13}^{+0.14}$	${}_{-0.12}^{+0.13}$	${}_{-0.05}^{+0.06}$
20–30	0.41	${}_{-0.10}^{+0.12}$	${}_{-0.10}^{+0.11}$	${}_{-0.04}^{+0.04}$
30–45	0.51	${}_{-0.10}^{+0.12}$	${}_{-0.10}^{+0.11}$	${}_{-0.04}^{+0.04}$
45–80	0.45	${}_{-0.09}^{+0.10}$	${}_{-0.09}^{+0.10}$	${}_{-0.03}^{+0.04}$
80–120	0.30	${}_{-0.07}^{+0.08}$	${}_{-0.07}^{+0.07}$	${}_{-0.02}^{+0.02}$
120–200	0.19	${}_{-0.05}^{+0.06}$	${}_{-0.05}^{+0.06}$	${}_{-0.01}^{+0.01}$
200–13000	0.03	${}_{-0.02}^{+0.02}$	${}_{-0.01}^{+0.02}$	${}_{-0.00}^{+0.00}$