Abstract

The production cross section of prompt $\mathrm{\Lambda_{c}^{+}}$ charm baryons was measured with the ALICE detector at the LHC at midrapidity in proton-proton (pp) and proton-lead (p-Pb) collisions at a centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}} = 5.02$ TeV. The $\mathrm{\Lambda_{c}^{+}}$ and $\rm {\overline{\Lambda}{}_c^-}$ baryons were reconstructed in the hadronic decay channels $\rm \Lambda_{c}^{+} \rightarrow p K^{-}\pi^{+}$ and $\rm \Lambda_{c}^{+}\to p K^{0}_{S}$ and respective charge conjugates. The measured differential cross sections as a function of transverse momentum ($p_{\rm T}$) and the $p_{\rm T}$-integrated $\mathrm{\Lambda_{c}^{+}}$ production cross section in pp and in p-Pb collisions are presented. The $\mathrm{\Lambda_{c}^{+}}$ nuclear modification factor ($R_\mathrm{pPb}$), calculated from the cross sections in pp and in p-Pb collisions, is presented and compared with the $R_\mathrm{pPb}$ of D mesons. The $\mathrm {\Lambda_{c}^{+}}/\mathrm {D^0}$ ratio is also presented and compared with the light-flavour baryon-to-meson ratios p$/\pi$ and $\Lambda /\mathrm {K^0_S}$, and measurements from other LHC experiments. The results are compared to predictions from model calculations and Monte Carlo event generators.

Highlights

  • In hadronic collisions, heavy quarks are created predominantly in hard scattering processes, and the measurement of charm and beauty hadron production is a powerful test of perturbative quantum chromodynamics calculations

  • This paper presents the measurement of the pT -differential production cross section of charm

  • The particle identification (PID) selections for all analyses were performed utilising the Bayesian method for combining the time projection chamber (TPC) and TOF signals, as described in Ref. [90]

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Summary

Introduction

Heavy quarks (charm and beauty) are created predominantly in hard scattering processes, and the measurement of charm and beauty hadron production is a powerful test of perturbative quantum chromodynamics (pQCD) calculations. Theoretical predictions based on the QCD factorization approach describe the heavy-flavor hadron production cross section as a convolution of parton distribution functions, parton hard-scattering cross sections, and fragmentation functions. B-meson production cross sections in pp collisions at centerof-mass energies between 200 GeV and 13 TeV at RHIC [1], Tevatron [2,3,4], and the LHC [5,6,7,8,9] are generally described within uncertainties by perturbative calculations at next-toleading order with next-to-leading-log resummation, such as the general-mass variable-flavor-number scheme + c production cross section relative to D mesons provide insight into the hadronization of charm quarks into baryons.

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