Table 2.

LO and NLO QCD inclusive cross sections for single B production at the LHC, running at a center-of-mass energy of $\sqrt{s}=13$ TeV. The results are shown together with the associated scale and PDF relative uncertainties in the context of several benchmark scenarios

$m_B$ [GeV]	Scenario	${\mathit{\sigma }}_{\mathrm{LO}}$ [pb]	${\mathit{\sigma }}_{\mathrm{NLO}}$ [pb]
400	BZ1	$(1.277{10}^0){}_{-3.0\%}^{+2.9\%}{}_{-2.6\%}^{+2.6\%}$	$(1.288{10}^0){}_{-0.4\%}^{+0.9\%}{}_{-2.6\%}^{+2.6\%}$
	BZ2	$(3.573{10}^0){}_{-1.3\%}^{+0.8\%}{}_{-4.8\%}^{+4.8\%}$	$(3.668{10}^0){}_{-0.3\%}^{+1.0\%}{}_{-4.7\%}^{+4.7\%}$
	BW1	$(2.021{10}^0){}_{-3.0\%}^{+2.9\%}{}_{-1.7\%}^{+1.7\%}$	$(2.033{10}^0){}_{-0.6\%}^{+0.9\%}{}_{-1.7\%}^{+1.7\%}$
	BW2	$(3.037{10}^0){}_{-0.7\%}^{+0.0\%}{}_{-1.4\%}^{+1.4\%}$	$(3.161{10}^0){}_{-0.7\%}^{+1.3\%}{}_{-1.4\%}^{+1.4\%}$
800	BZ1	$(3.197{10}^{-1}){}_{-5.9\%}^{+6.6\%}{}_{-3.3\%}^{+3.3\%}$	$(3.461{10}^{-1}){}_{-1.2\%}^{+1.0\%}{}_{-3.2\%}^{+3.2\%}$
	BZ2	$(6.777{10}^{-1}){}_{-4.6\%}^{+4.9\%}{}_{-8.0\%}^{+8.0\%}$	$(7.671{10}^{-1}){}_{-1.3\%}^{+1.4\%}{}_{-7.4\%}^{+7.4\%}$
	BW1	$(5.450{10}^{-1}){}_{-5.8\%}^{+6.4\%}{}_{-1.8\%}^{+1.8\%}$	$(5.858{10}^{-1}){}_{-1.1\%}^{+1.0\%}{}_{-1.8\%}^{+1.8\%}$
	BW2	$(5.335{10}^{-1}){}_{-3.5\%}^{+3.4\%}{}_{-2.0\%}^{+2.0\%}$	$(5.938{10}^{-1}){}_{-0.8\%}^{+1.4\%}{}_{-1.8\%}^{+1.8\%}$
1200	BZ1	$(1.129{10}^{-1}){}_{-7.6\%}^{+8.8\%}{}_{-4.2\%}^{+4.2\%}$	$(1.291{10}^{-1}){}_{-2.3\%}^{+1.7\%}{}_{-4.0\%}^{+4.0\%}$
	BZ2	$(1.966{10}^{-1}){}_{-6.5\%}^{+7.2\%}{}_{-12.6\%}^{+12.6\%}$	$(2.268{10}^{-1}){}_{-2.0\%}^{+1.7\%}{}_{-11.8\%}^{+11.8\%}$
	BW1	$(2.021{10}^{-1}){}_{-7.3\%}^{+8.5\%}{}_{-2.0\%}^{+2.0\%}$	$(2.298{10}^{-1}){}_{-2.1\%}^{+1.5\%}{}_{-2.1\%}^{+2.1\%}$
	BW2	$(1.406{10}^{-1}){}_{-5.4\%}^{+5.7\%}{}_{-3.3\%}^{+3.3\%}$	$(1.645{10}^{-1}){}_{-1.8\%}^{+1.8\%}{}_{-3.1\%}^{+3.1\%}$
1600	BZ1	$(4.607{10}^{-2}){}_{-8.8\%}^{+10.3\%}{}_{-5.2\%}^{+5.2\%}$	$(5.519{10}^{-2}){}_{-3.1\%}^{+2.6\%}{}_{-4.9\%}^{+4.9\%}$
	BZ2	$(6.934{10}^{-2}){}_{-7.8\%}^{+8.9\%}{}_{-18.9\%}^{+18.9\%}$	$(8.316{10}^{-2}){}_{-2.8\%}^{+2.5\%}{}_{-17.6\%}^{+17.6\%}$
	BW1	$(8.603{10}^{-2}){}_{-8.5\%}^{+9.9\%}{}_{-2.4\%}^{+2.4\%}$	$(1.022{10}^{-1}){}_{-3.0\%}^{+2.4\%}{}_{-2.4\%}^{+2.4\%}$
	BW2	$(4.447{10}^{-2}){}_{-6.7\%}^{+7.4\%}{}_{-5.1\%}^{+5.1\%}$	$(5.423{10}^{-2}){}_{-2.6\%}^{+2.5\%}{}_{-4.7\%}^{+4.7\%}$
2000	BZ1	$(2.022{10}^{-2}){}_{-9.7\%}^{+11.6\%}{}_{-6.4\%}^{+6.4\%}$	$(2.516{10}^{-2}){}_{-3.9\%}^{+3.3\%}{}_{-6.1\%}^{+6.1\%}$
	BZ2	$(2.751{10}^{-2}){}_{-8.7\%}^{+10.2\%}{}_{-26.9\%}^{+26.9\%}$	$(3.412{10}^{-2}){}_{-3.5\%}^{+3.2\%}{}_{-25.1\%}^{+25.1\%}$
	BW1	$(3.922{10}^{-2}){}_{-9.4\%}^{+11.2\%}{}_{-2.9\%}^{+2.9\%}$	$(4.873{10}^{-2}){}_{-3.8\%}^{+3.3\%}{}_{-2.8\%}^{+2.8\%}$
	BW2	$(1.564{10}^{-2}){}_{-7.8\%}^{+8.8\%}{}_{-7.3\%}^{+7.3\%}$	$(1.981{10}^{-2}){}_{-3.3\%}^{+3.2\%}{}_{-6.9\%}^{+6.9\%}$