Table 1.

Values of the $\mathrm{p}\mathrm{p}\to H\to \mathit{\gamma }\mathit{\gamma }$ differential cross sections as a function of kinematic observables as measured in data and as predicted in SM simulations. For each observable the fit to $m_{\mathit{\gamma }\mathit{\gamma }}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit ${\widehat{m}}_H$ varies from observable to observable

	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.4\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{H}\mathrm{R}\mathrm{E}\mathrm{S}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
Fiducial cross section	$32.2_{-9.7}^{+10.1}$	$30.3_{-4.7}^{+5.9}$	$31.5_{-3.0}^{+4.0}$	$32.0_{-4.6}^{+5.8}$
$p_{\mathrm{T}}^{\mathit{\gamma }\mathit{\gamma }}$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.8\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{H}\mathrm{R}\mathrm{E}\mathrm{S}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0–$15\text{GeV}$	$9.0_{-6.2}^{+6.4}$	$7.5_{-1.2}^{+1.5}$	$8.6_{-0.9}^{+0.9}$	$8.6_{-1.3}^{+1.6}$
15–$26\text{GeV}$	$2.0_{-5.5}^{+4.9}$	$5.9_{-1.0}^{+1.2}$	$6.8_{-0.7}^{+0.8}$	$6.6_{-1.0}^{+1.3}$
26–$43\text{GeV}$	$3.4_{-4.6}^{+4.8}$	$6.1_{-1.0}^{+1.3}$	$6.3_{-0.7}^{+1.0}$	$6.2_{-0.9}^{+1.1}$
43–$72\text{GeV}$	$6.2_{-3.5}^{+3.7}$	$5.2_{-0.9}^{+1.1}$	$5.2_{-0.6}^{+0.9}$	$5.1_{-0.7}^{+0.9}$
72–$125\text{GeV}$	$4.6_{-2.7}^{+2.4}$	$3.4_{-0.6}^{+0.7}$	$3.3_{-0.4}^{+0.6}$	$3.3_{-0.4}^{+0.6}$
125–$200\text{GeV}$	$2.6_{-1.0}^{+1.0}$	$1.4_{-0.2}^{+0.3}$	$1.3_{-0.3}^{+0.3}$	$1.3_{-0.2}^{+0.2}$
$>$200$\text{GeV}$	$0.7_{-0.4}^{+0.5}$	$0.6_{-0.1}^{+0.1}$	$0.5_{-0.1}^{+0.1}$	$0.6_{-0.1}^{+0.2}$

$|cos{\mathit{\theta }}^{\ast }|$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.7\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{H}\mathrm{R}\mathrm{E}\mathrm{S}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0.00–0.11	$4.9_{-3.3}^{+3.3}$	$4.3_{-0.7}^{+0.8}$	$4.8_{-0.5}^{+0.5}$	$4.6_{-0.7}^{+0.8}$
0.11–0.23	$3.3_{-3.1}^{+3.2}$	$4.7_{-0.7}^{+0.9}$	$5.2_{-0.6}^{+0.7}$	$5.0_{-0.7}^{+0.9}$
0.23–0.36	$11.7_{-3.5}^{+3.8}$	$4.9_{-0.8}^{+1.0}$	$5.4_{-0.5}^{+0.7}$	$5.2_{-0.7}^{+0.9}$
0.36–0.53	$2.4_{-5.1}^{+5.6}$	$6.1_{-1.0}^{+1.2}$	$6.7_{-0.6}^{+0.9}$	$6.4_{-0.9}^{+1.2}$
0.53–1.00	$7.3_{-7.1}^{+7.3}$	$10.2_{-1.6}^{+2.0}$	$9.6_{-1.0}^{+1.4}$	$10.7_{-1.5}^{+2.0}$

$\mathrm{\Delta }{\mathit{\varphi }}^{\mathit{\gamma }\mathit{\gamma }}$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.6\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{H}\mathrm{R}\mathrm{E}\mathrm{S}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0.00–0.92	$0.9_{-0.8}^{+0.9}$	$1.1_{-0.2}^{+0.2}$	$0.9_{-0.1}^{+0.1}$	$1.0_{-0.1}^{+0.2}$
0.92–1.72	$2.6_{-1.6}^{+1.4}$	$2.2_{-0.3}^{+0.4}$	$2.0_{-0.2}^{+0.3}$	$2.1_{-0.3}^{+0.4}$
1.72–2.37	$2.2_{-2.5}^{+2.6}$	$4.2_{-0.7}^{+0.9}$	$4.0_{-0.5}^{+0.7}$	$4.2_{-0.5}^{+0.7}$
2.37–2.74	$8.2_{-3.9}^{+4.1}$	$5.9_{-1.0}^{+1.2}$	$5.9_{-0.7}^{+0.9}$	$5.9_{-0.8}^{+1.1}$
2.74–2.97	$2.8_{-5.4}^{+4.4}$	$7.4_{-1.2}^{+1.5}$	$8.2_{-0.7}^{+1.1}$	$8.2_{-1.2}^{+1.5}$
2.97–3.15	$14.4_{-6.6}^{+9.0}$	$9.4_{-1.5}^{+1.9}$	$10.5_{-1.3}^{+1.0}$	$10.6_{-1.6}^{+2.0}$

$||y^{\mathit{\gamma }\mathit{\gamma }}||$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.2\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{H}\mathrm{R}\mathrm{E}\mathrm{S}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0.00–0.16	$2.4_{-2.6}^{+2.6}$	$3.1_{-0.5}^{+0.6}$	$3.2_{-0.3}^{+0.4}$	$3.2_{-0.5}^{+0.6}$
0.16–0.35	$2.2_{-2.6}^{+2.7}$	$3.7_{-0.6}^{+0.7}$	$3.7_{-0.4}^{+0.5}$	$3.9_{-0.6}^{+0.7}$
0.35–0.58	$9.5_{-3.2}^{+3.3}$	$4.3_{-0.7}^{+0.8}$	$4.4_{-0.5}^{+0.6}$	$4.5_{-0.7}^{+0.8}$
0.58–0.90	$5.4_{-3.7}^{+4.5}$	$5.6_{-0.9}^{+1.1}$	$5.9_{-0.6}^{+0.9}$	$5.8_{-0.8}^{+1.1}$
0.90–2.50	$15.9_{-11.1}^{+11.9}$	$13.8_{-2.1}^{+2.7}$	$14.4_{-1.3}^{+1.8}$	$14.7_{-2.1}^{+2.7}$

$N_{\text{jets}}$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.6\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}}$ ${}_{\mathrm{HJ}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0	$20.2_{-9.0}^{+9.3}$	$17.4_{-2.8}^{+3.5}$	$18.1_{-2.5}^{+6.0}$	$19.0_{-2.8}^{+3.6}$
1	$4.3_{-6.3}^{+6.4}$	$8.7_{-1.5}^{+1.8}$	$9.6_{-1.3}^{+2.2}$	$9.2_{-1.3}^{+1.7}$
2	$3.9_{-3.8}^{+3.7}$	$3.1_{-0.5}^{+0.6}$	$3.1_{-0.4}^{+0.7}$	$2.8_{-0.3}^{+0.5}$
$\ge$3	$2.5_{-2.2}^{+2.2}$	$1.1_{-0.2}^{+0.2}$	$1.0_{-0.1}^{+0.3}$	$1.0_{-0.1}^{+0.2}$

$p_{\mathrm{T}}^{\mathrm{j}1}$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.3\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}}$ ${}_{\mathrm{HJ}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
25–$40\text{GeV}$	$2.1_{-6.6}^{+6.8}$	$4.4_{-0.8}^{+1.0}$	$4.5_{-0.6}^{+1.2}$	$4.5_{-0.6}^{+0.8}$
40–$64\text{GeV}$	$6.4_{-5.0}^{+5.6}$	$3.7_{-0.7}^{+0.8}$	$3.9_{-0.5}^{+0.9}$	$3.8_{-0.5}^{+0.6}$
64–$104\text{GeV}$	$3.4_{-3.3}^{+3.4}$	$2.7_{-0.4}^{+0.5}$	$2.9_{-0.4}^{+0.6}$	$2.7_{-0.3}^{+0.4}$
104–$200\text{GeV}$	$0.8_{-1.8}^{+1.9}$	$1.6_{-0.2}^{+0.3}$	$1.8_{-0.3}^{+0.4}$	$1.6_{-0.2}^{+0.3}$
$>$200$\text{GeV}$	$0.8_{-0.7}^{+0.8}$	$0.4_{-0.1}^{+0.1}$	$0.5_{-0.1}^{+0.1}$	$0.4_{-0.1}^{+0.1}$

$|y^{\mathit{\gamma }\mathit{\gamma }}-y^{\mathrm{j}1}|$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.5\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}}$ ${}_{\mathrm{HJ}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0.00–0.62	$6.1_{-3.8}^{+4.0}$	$3.8_{-0.6}^{+0.7}$	$4.0_{-0.5}^{+0.9}$	$3.7_{-0.5}^{+0.6}$
0.62–1.25	$-1.1_{-3.6}^{+4.4}$	$3.4_{-0.6}^{+0.7}$	$3.6_{-0.5}^{+0.8}$	$3.4_{-0.5}^{+0.6}$
1.25–1.92	$5.2_{-2.8}^{+3.0}$	$2.7_{-0.5}^{+0.5}$	$2.9_{-0.4}^{+0.7}$	$2.7_{-0.4}^{+0.5}$
$>$1.92	$1.6_{-4.8}^{+4.1}$	$3.0_{-0.5}^{+0.6}$	$3.2_{-0.5}^{+0.7}$	$3.1_{-0.4}^{+0.5}$

$m_{\mathrm{jj}}$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.7\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}}$ ${}_{\mathrm{HJ}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0–$153\text{GeV}$	$6.8_{-4.0}^{+4.5}$	$3.0_{-0.6}^{+0.7}$	$2.9_{-0.4}^{+0.7}$	$2.6_{-0.3}^{+0.4}$
153–$455\text{GeV}$	$1.8_{-3.2}^{+3.0}$	$2.1_{-0.4}^{+0.4}$	$2.1_{-0.3}^{+0.5}$	$2.0_{-0.2}^{+0.3}$
455–$1000\text{GeV}$	$0.3_{-1.0}^{+1.2}$	$0.8_{-0.1}^{+0.1}$	$0.9_{-0.1}^{+0.1}$	$0.8_{-0.1}^{+0.1}$
$>$1000$\text{GeV}$	$-0.2_{-0.2}^{+0.3}$	$0.3_{-0.0}^{+0.0}$	$0.3_{-0.0}^{+0.0}$	$0.3_{-0.0}^{+0.0}$

$\mathrm{\Delta }{\mathit{\eta }}^{\mathrm{jj}}$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.4\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}}$ ${}_{\mathrm{HJ}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0.00–1.65	$3.0_{-3.5}^{+3.6}$	$2.9_{-0.5}^{+0.6}$	$2.8_{-0.4}^{+0.7}$	$2.5_{-0.3}^{+0.4}$
1.65–4.30	$3.7_{-2.6}^{+2.8}$	$2.4_{-0.4}^{+0.5}$	$2.3_{-0.3}^{+0.5}$	$2.2_{-0.3}^{+0.3}$
4.30–10.00	$0.1_{-0.9}^{+1.0}$	$0.9_{-0.1}^{+0.1}$	$0.9_{-0.1}^{+0.1}$	$0.9_{-0.1}^{+0.1}$

$\mathrm{\Delta }{\mathit{\varphi }}^{\mathit{\gamma }\mathit{\gamma },\mathrm{jj}}$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.5\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}}$ ${}_{\mathrm{HJ}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0.00–2.95	$-0.1_{-0.2}^{+0.2}$	$0.1_{-0.0}^{+0.0}$	$0.1_{-0.0}^{+0.0}$	$0.1_{-0.0}^{+0.0}$
2.95–3.08	$9.6_{-4.3}^{+5.0}$	$1.9_{-0.3}^{+0.4}$	$1.9_{-0.3}^{+0.4}$	$1.8_{-0.2}^{+0.3}$
3.08–3.15	$-1.1_{-2.8}^{+2.5}$	$1.6_{-0.2}^{+0.2}$	$1.7_{-0.2}^{+0.3}$	$1.6_{-0.2}^{+0.2}$

$\mathrm{\Delta }{\mathit{\varphi }}^{\mathrm{jj}}$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.6\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}}$ ${}_{\mathrm{HJ}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0.00–0.88	$1.5_{-1.9}^{+2.0}$	$1.6_{-0.3}^{+0.3}$	$1.7_{-0.2}^{+0.3}$	$1.4_{-0.2}^{+0.2}$
0.88–1.82	$1.1_{-2.3}^{+2.1}$	$1.7_{-0.3}^{+0.3}$	$1.6_{-0.2}^{+0.3}$	$1.6_{-0.2}^{+0.3}$
1.82–3.15	$5.0_{-3.5}^{+3.8}$	$3.0_{-0.5}^{+0.6}$	$2.8_{-0.4}^{+0.7}$	$2.7_{-0.3}^{+0.4}$

$|{\mathit{\eta }}^{\mathit{\gamma }\mathit{\gamma }}-({\mathit{\eta }}^{\mathrm{j}1}+{\mathit{\eta }}^{\mathrm{j}2})/2|$	${\mathit{\sigma }}_{\text{obs}}[\text{fb}]$ $({\widehat{m}}_H=124.6\text{GeV})$	${\mathit{\sigma }}_{\mathrm{M}\mathrm{A}\mathrm{D}\mathrm{G}\mathrm{R}\mathrm{A}\mathrm{P}\mathrm{H}5\_a\mathrm{M}\mathrm{C}@\mathrm{N}\mathrm{L}\mathrm{O}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}}$ ${}_{\mathrm{HJ}+\mathrm{XH}}$	${\mathit{\sigma }}_{\mathrm{P}\mathrm{O}\mathrm{W}\mathrm{H}\mathrm{E}\mathrm{G}+\mathrm{XH}}$
0.0–0.5	$1.6_{-2.1}^{+1.8}$	$1.6_{-0.2}^{+0.3}$	$1.6_{-0.2}^{+0.3}$	$1.5_{-0.2}^{+0.2}$
0.5–1.2	$5.8_{-2.2}^{+2.4}$	$1.9_{-0.3}^{+0.4}$	$1.9_{-0.2}^{+0.4}$	$1.7_{-0.2}^{+0.3}$
$>$1.2	$-0.1_{-3.7}^{+3.8}$	$2.6_{-0.5}^{+0.6}$	$2.6_{-0.3}^{+0.6}$	$2.4_{-0.3}^{+0.4}$