Charm fragmentation fractions and ${\rm c\overline{c}}$ cross section in p$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV

The total charm-quark production cross section per unit of rapidity $\mathrm{d}\sigma({\rm c\overline{c}})/\mathrm{d}y$, and the fragmentation fractions of charm quarks to different charm-hadron species $f(\mathrm{c}\rightarrow {\rm h_{c}})$, are measured for the first time in p$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV at midrapidity ($-0.96<~y<~0.04$ in the centre-of-mass frame) using data collected by ALICE at the CERN LHC. The results are obtained based on all the available measurements of prompt production of ground-state charm-hadron species: $\mathrm{D}^{0}$, $\mathrm{D}^{+}$, $\mathrm{D}_\mathrm{s}^{+}$, and $\mathrm{J/\psi}$ mesons, and $\Lambda_\mathrm{c}^{+}$ and $\Xi_{\rm c}^{0}$ baryons. The resulting cross section is $\mathrm{d}\sigma({\rm c\overline{c}})/\mathrm{d}y =219.6 \pm 6.3\;(\mathrm{stat.}) {\;}_{-11.8}^{+10.5}\;(\mathrm{syst.}) {\;}_{-2.9}^{+7.6}\;(\mathrm{extr.})\pm 5.4\;(\mathrm{BR})\pm 4.6\;(\mathrm{lumi.}) \pm 19.5\;(\text{rapidity shape})+15.0\;(\Omega_{\rm c}^{0})$ mb, which is consistent with a binary scaling of pQCD calculations from pp collisions. The measured fragmentation fractions are compatible with those measured in pp collisions at $\sqrt{s} = 5.02$ and $13$ TeV, showing an increase in the relative production rates of charm baryons with respect to charm mesons in pp and p$-$Pb collisions compared with $\mathrm{e^{+}e^{-}}$ and $\mathrm{e^{-}p}$ collisions. The $p_\mathrm{T}$-integrated nuclear modification factor of charm quarks, $R_\mathrm{pPb}({\rm c\overline{c}})= 0.91 \pm 0.04\;{\rm (stat.)}{}^{+0.08}_{-0.09}\;{\rm (syst.)}{}^{+0.04}_{-0.03}\;{\rm (extr.)}{}\pm 0.03\;{\rm (lumi.)}$, is found to be consistent with unity and with theoretical predictions including nuclear modifications of the parton distribution functions.

 

Submitted to: EPJC
e-Print: arXiv:2405.14571 | PDF | inSPIRE
CERN-EP-2024-141
Figure group

Figure 1

Left: The fragmentation fractions for charm hadrons in p–Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02\,\mathrm{TeV}$, compared with results from pp collisions at $\sqrt{s}=5.02\,\mathrm{TeV}$ and from $\mathrm{e^+e^-}$ and $\mathrm{e^-p}$ collisions at lower energies. The fragmentation fractions for $\mathrm{J}/\psi$ are multiplied by 20 for visibility. Right: Total $\mathrm{c\overline{c}}$ production cross section per unit of rapidity and per nucleon in p–Pb collisions, compared with measurements in pp collisions from ALICE, PHENIX, and STAR, and with FONLL and NNLO pQCD calculations. The statistical uncertainties are shown as bars, and the systematic uncertainties as unfilled boxes.

Figure 2

The $p_\mathrm{T}$-integrated nuclear modification factor $R_\mathrm{pPb}$ for $\mathrm{D}^0$ mesons, $\Lambda_\mathrm{c}^{+}$ baryons, $\mathrm{J}/\psi$ mesons, and $\mathrm{c\overline{c}}$ pairs in p–Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02\,\mathrm{TeV}$. The results are compared with calculations using the nCTEQ15$_{\mathrm{rwHF}}$ (yellow shaded band) and EPPS16 (blue crosshatched band) nPDF sets. The horizontal lines represent the central values of the respective predictions.