Table 4.

Full set of kinematical cuts applied to the processes used for NNPDF3.1 PDF determination at NLO and at NNLO. Only data satisfying the constraints in the table are retained. The experiments in brackets are not part of the global dataset and only used for dedicated studies. The cut on the HERA charm structure function data at NNLO is applied only when charm is fitted, and it is applied in addition to the other DIS kinematical cuts

Dataset	NLO	NNLO
DIS structure functions	$W^2\ge 12.5$ GeV${}^2$	$W^2\ge 12.5$ GeV${}^2$
	$Q^2\ge 3.5$ GeV${}^2$	$Q^2\ge 3.5$ GeV${}^2$
HERA ${\mathit{\sigma }}_c^{\mathrm{NC}}$ (in addition)	–	$Q^2\ge 8$ GeV${}^2$ (fitted charm)
ATLAS 7 TeV inclusive jets 2011	$|y_{\mathrm{jet}}|\le 0.4$	$|y_{\mathrm{jet}}|\le 0.4$
Drell–Yan E605 and E866	$\mathit{\tau }\le 0.080$	$\mathit{\tau }\le 0.080$
	$|y/y_{\max }|\le 0.663$	$|y/y_{\max }|\le 0.663$
D0 $W\to l\mathit{\nu }$ asymmetries	–	$|A_l|\ge 0.03$
CMS Drell–Yan 2D 7 TeV	30 GeV $\le M_{ll}\le 200$ GeV	$M_{ll}\le 200$ GeV
	$|y_Z|\le 2.2$	$|y_Z|\le 2.2$
[CMS Drell–Yan 2D 8 TeV]	$M_{ll}\ge 30$ GeV	$M_{ll}\ge 30$ GeV
LHCb 7 TeV and 8 TeV $W,Z\to \mathit{\mu }$	–	$|y_l|\ge 2.25$
[ATLAS $Z{p}_T$ 7 TeV]	$30\mathrm{GeV}\le p_T^Z\le 500\mathrm{GeV}$	$30\mathrm{GeV}\le p_T^Z\le 500\mathrm{GeV}$
ATLAS $Z{p}_T$ 8 TeV $(p_T,M_{ll})$	$p_T^Z\ge 30\mathrm{GeV}$	$p_T^Z\ge 30\mathrm{GeV}$
ATLAS $Z{p}_T$ 8 TeV $(p_T,y_Z)$	$30\mathrm{GeV}\le p_T^Z\le 150\mathrm{GeV}$	$30\mathrm{GeV}\le p_T^Z\le 150\mathrm{GeV}$
CMS $Z{p}_T$ 8 TeV $(p_T,y_Z)$	$30\mathrm{GeV}\le p_T^Z\le 170\mathrm{GeV}$	$30\mathrm{GeV}\le p_T^Z\le 170\mathrm{GeV}$
	$|y_Z|\le 1.6$	$|y_Z|\le 1.6$