Figure 2

Product of detector acceptance and efficiency for $\Xi_{\rm c}^{0}$ baryons in p-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV as a function of $p_{\rm T}$. The solid line corresponds to the $(\mathrm{Acc}\times\epsilon)$ for prompt $\Xi_{\rm c}^{0}$, while the dotted line represents $(\mathrm{Acc}\times\epsilon)$ for $\Xi_{\rm c}^{0}$ baryons originating from beauty-hadron decays. The statistical uncertainties are smaller than the marker size.