Abstract

In relativistic nuclear collisions the production of hadrons with light (u,d,s) quarks is quantitatively described in the framework of the Statistical Hadronization Model (SHM). Charm quarks are dominantly produced in initial hard collisions but interact strongly in the hot fireball and thermalize. Therefore charmed hadrons can be incorporated into the SHM by treating charm quarks as ‘impurities’ with thermal distributions, while the total charm content of the fireball is fixed by the measured open charm cross section. We call this model SHMc and demonstrate that with SHMc the measured multiplicities of single charm hadrons in lead-lead collisions at LHC energies can be well described with the same thermal parameters as for (u,d,s) hadrons. Furthermore, transverse momentum distributions are computed in a blast-wave model, which includes the resonance decay kinematics. SHMc is extended to lighter collision systems down to oxygen-oxygen and includes doubly- and triply-charmed hadrons. We show predictions for production probabilities of such states exhibiting a characteristic and quite spectacular enhancement hierarchy.

Highlights

  • Follows: the charm quark mass mc is much larger than Tpc and thermal production of charm quarks or hadrons is strongly Boltzmann suppressed

  • Charmed hadrons can be incorporated into the Statistical Hadronization Model (SHM) by treating charm quarks as ‘impurities’ with thermal distributions, while the total charm content of the fireball is fixed by the measured open charm cross section

  • We show the comparison between the SHMc predictions and data for spectra and nuclear modification factor RAA as a function of transverse momentum pT

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Summary

Heavy quarks in the statistical hadronization model

We recapitulate the physics ideas and formalism behind the SHMc with special focus on the multi-charm sector. The large value of gc = 29.6 ± 5.2 for central Pb-Pb collisions for charm production at mid-rapidity (see figure 1 ) implies very large enhancements for charmed hadrons compared to what is obtained in the purely thermal case. Correction factors are close to 1: 0.98, 0.92, and 0.84 for α = 1, 2, 3 charm quarks respectively, for the central value of the differential charm cross section at mid-rapidity, see figure 2 below If these enhancement factors are realized in nature even very massive triply charmed hadrons may come into reach experimentally.

Dependence on mass number of the colliding nuclei
The canonical volume
Charm hadron production and deconfinement of charm quarks
Charm hadron spectrum and SHMc
Transverse momentum spectra of charm hadrons
Results for Pb-Pb and lighter collision systems
Transverse momentum distributions
Integrated yields
Conclusions and outlook
Full Text
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