Figure 2

Product of detector acceptance and efficiency for \Lc baryons in pp collisions at $\sqrt{s}=5.02 \TeV$, as a function of \pt. From left to right: \LctopKpi and \LctopKzS. The solid lines correspond to the $(A\times\varepsilon)$ for prompt \Lc, while the dotted lines represent $(A \times \epsilon)$ for \Lc baryons originating from beauty-hadron decays. The statistical uncertainties are smaller than the marker size.