Table 2.

Measured and predicted differential cross section for isolated-photon production, along with the statistical and systematical uncertainties in the various $E_{\mathrm{T}}$ and y bins. Predictions use jetphox  at NLO with the NNPDF3.0 PDF set. The ratio of the jetphox  predictions to data are listed in the last column, with the total uncertainty estimated assuming uncorrelated experimental and theoretical uncertainties

$E_{\mathrm{T}}$ ($\text{GeV}$ )	Measured cross section within the bin (pb)	jetphox NNPDF3.0 (pb)	jetphox/Data
$|y^{\gamma }|<0.8$
190–200	$(3.64\pm 0.04\text{(stat)}\pm 0.23\text{(syst)})\times {10}^{-1}$	($3.1\pm 0.3)\times {10}^{-1}$	$0.85\pm 0.10$
200–220	$(2.49\pm 0.02\text{(stat)}\pm 0.15\text{(syst)})\times {10}^{-1}$	($2.2\pm 0.2)\times {10}^{-1}$	$0.88\pm 0.09$
220–250	$(1.46\pm 0.01\text{(stat)}\pm 0.09\text{(syst)})\times {10}^{-1}$	($1.3\pm 0.1)\times {10}^{-1}$	$0.90\pm 0.10$
250–300	$(7.09\pm 0.08\text{(stat)}\pm 0.45\text{(syst)})\times {10}^{-2}$	($6.4\pm 0.5)\times {10}^{-2}$	$0.91\pm 0.10$
300–350	$(2.91\pm 0.05\text{(stat)}\pm 0.19\text{(syst)})\times {10}^{-2}$	($2.7\pm 0.3)\times {10}^{-2}$	$0.92\pm 0.12$
350–400	$(1.24\pm 0.03\text{(stat)}\pm 0.10\text{(syst)})\times {10}^{-2}$	($1.4\pm 0.2)\times {10}^{-2}$	$1.11\pm 0.15$
400–500	$(5.1\pm 0.1\text{(stat)}\pm 0.4\text{(syst)})\times {10}^{-3}$	($5.0\pm 0.6)\times {10}^{-3}$	$0.98\pm 0.14$
500–750	$(1.11\pm 0.04\text{(stat)}\pm 0.08\text{(syst)})\times {10}^{-3}$	($9.0\pm 1.0)\times {10}^{-4}$	$0.79\pm 0.14$
750–1000	$(1.0\pm 0.1\text{(stat)}\pm 0.1\text{(syst)})\times {10}^{-4}$	($1.4\pm 0.4)\times {10}^{-4}$	$1.33\pm 0.44$
$0.8<|y^{\gamma }|<1.44$
190–200	$(3.44\pm 0.04\text{(stat)}\pm 0.25\text{(syst)})\times {10}^{-1}$	($3.0\pm 0.3)\times {10}^{-1}$	$0.88\pm 0.10$
200–220	$(2.26\pm 0.03\text{(stat)}\pm 0.18\text{(syst)})\times {10}^{-1}$	($2.1\pm 0.2)\times {10}^{-1}$	$0.95\pm 0.12$
220–250	$(1.37\pm 0.02\text{(stat)}\pm 0.09\text{(syst)})\times {10}^{-1}$	($1.3\pm 0.1)\times {10}^{-1}$	$0.94\pm 0.10$
250–300	$(5.87\pm 0.08\text{(stat)}\pm 0.40\text{(syst)})\times {10}^{-2}$	($6.2\pm 0.6)\times {10}^{-2}$	$1.06\pm 0.12$
300–350	$(2.60\pm 0.05\text{(stat)}\pm 0.17\text{(syst)})\times {10}^{-2}$	($2.7\pm 0.2)\times {10}^{-2}$	$1.04\pm 0.12$
350–400	$(1.15\pm 0.04\text{(stat)}\pm 0.09\text{(syst)})\times {10}^{-2}$	($1.3\pm 0.1)\times {10}^{-2}$	$1.15\pm 0.13$
400–500	$(4.6\pm 0.2\text{(stat)}\pm 0.3\text{(syst)})\times {10}^{-3}$	($4.7\pm 0.5)\times {10}^{-3}$	$1.04\pm 0.13$
500–750	$(7.4\pm 0.4\text{(stat)}\pm 0.6\text{(syst)})\times {10}^{-4}$	($8.2\pm 0.8)\times {10}^{-4}$	$1.11\pm 0.15$
750–1000	$(8.0\pm 1.0\text{(stat)}\pm 1.0\text{(syst)})\times {10}^{-5}$	($1.1\pm 0.2)\times {10}^{-4}$	$1.40\pm 0.39$
$1.57<|y^{\gamma }|<2.1$
190–200	$(3.16\pm 0.05\text{(stat)}\pm 0.31\text{(syst)})\times {10}^{-1}$	($2.8\pm 0.3)\times {10}^{-1}$	$0.88\pm 0.13$
200–220	$(2.19\pm 0.03\text{(stat)}\pm 0.19\text{(syst)})\times {10}^{-1}$	($2.0\pm 0.2)\times {10}^{-1}$	$0.91\pm 0.12$
220–250	$(1.19\pm 0.02\text{(stat)}\pm 0.12\text{(syst)})\times {10}^{-1}$	($1.1\pm 0.1)\times {10}^{-1}$	$0.96\pm 0.13$
250–300	$(5.80\pm 0.09\text{(stat)}\pm 0.54\text{(syst)})\times {10}^{-2}$	($5.4\pm 0.5)\times {10}^{-2}$	$0.92\pm 0.12$
300–350	$(2.37\pm 0.06\text{(stat)}\pm 0.22\text{(syst)})\times {10}^{-2}$	($2.2\pm 0.3)\times {10}^{-2}$	$0.93\pm 0.14$
350–400	$(1.02\pm 0.04\text{(stat)}\pm 0.12\text{(syst)})\times {10}^{-2}$	($9.5\pm 0.9)\times {10}^{-3}$	$0.93\pm 0.15$
400–500	$(4.0\pm 0.2\text{(stat)}\pm 0.5\text{(syst)})\times {10}^{-3}$	($3.1\pm 0.3)\times {10}^{-3}$	$0.77\pm 0.13$
500–750	$(6.1\pm 0.4\text{(stat)}\pm 0.9\text{(syst)})\times {10}^{-4}$	($4.6\pm 0.5)\times {10}^{-4}$	$0.76\pm 0.14$
750–1000	$(3.9\pm 1.0\text{(stat)}\pm 1.1\text{(syst)})\times {10}^{-5}$	($3.0\pm 0.9)\times {10}^{-5}$	$0.78\pm 0.37$
$2.1<|y^{\gamma }|<2.5$
190–200	$(2.52\pm 0.07\text{(stat)}\pm 0.35\text{(syst)})\times {10}^{-1}$	($2.3\pm 0.3)\times {10}^{-1}$	$0.92\pm 0.17$
200–220	$(1.55\pm 0.04\text{(stat)}\pm 0.14\text{(syst)})\times {10}^{-1}$	($1.6\pm 0.2)\times {10}^{-1}$	$1.04\pm 0.14$
220–250	$(8.8\pm 0.2\text{(stat)}\pm 0.8\text{(syst)})\times {10}^{-2}$	($9.0\pm 1.0)\times {10}^{-2}$	$1.02\pm 0.15$
250–300	$(3.7\pm 0.1\text{(stat)}\pm 0.4\text{(syst)})\times {10}^{-2}$	($3.8\pm 0.4)\times {10}^{-2}$	$1.01\pm 0.14$
300–350	$(1.32\pm 0.07\text{(stat)}\pm 0.15\text{(syst)})\times {10}^{-2}$	($1.4\pm 0.1)\times {10}^{-2}$	$1.06\pm 0.17$
350–400	$(5.9\pm 0.4\text{(stat)}\pm 0.7\text{(syst)})\times {10}^{-3}$	($5.0\pm 0.5)\times {10}^{-3}$	$0.85\pm 0.14$
400–500	$(1.7\pm 0.1\text{(stat)}\pm 0.3\text{(syst)})\times {10}^{-3}$	($1.2\pm 0.1)\times {10}^{-3}$	$0.72\pm 0.16$
500–750	$(1.8\pm 0.2\text{(stat)}\pm 0.4\text{(syst)})\times {10}^{-4}$	($1.4\pm 0.3)\times {10}^{-4}$	$0.77\pm 0.25$