QM 2022

Charm production: constraint to transport models and charm diffusion coefficient with ALICE

7 Apr 2022, 09:00

20m

medium aula B (Auditorium Maximum UJ)

Oral presentation Heavy flavors, quarkonia, and strangeness production Parallel Session T11: Heavy flavors, quarkonia, and strangeness production

Speaker

Lucas Anne Vermunt (Utrecht University (NL))

Description

In this contribution the nuclear modification factor ($R_{\mathrm{AA}}$) of prompt charm hadrons and heavy-flavour hadrons decaying to leptons measured in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV by the ALICE Collaboration are presented. The measurement of heavy-flavour leptons in Xe-Xe collisions is also discussed. Heavy quarks are a very suitable probe to investigate the quark-gluon plasma (QGP) produced in heavy-ion collisions, since they are mainly produced in hard-scattering processes and hence in shorter timescales compared to the QGP. Measurements of charm-hadron production in nucleus-nucleus collisions are therefore useful to study the properties of the in-medium charm-quark energy loss via the comparison with theoretical models. Moreover, the comparison of different colliding systems provides insights in the dependency on the collision geometry.
Models describing the heavy-flavour transport and energy loss in an hydrodynamically expanding QGP require also a precise modelling of the in-medium hadronisation of heavy quarks, which is investigated via the measurement of prompt ${\mathrm{D}}_{\mathrm{s}}^{+}$ mesons and ${\mathrm{\Lambda }}_{\mathrm{c}}^{+}$ baryons.
In addition, the measurement of the azimuthal anisotropy of strange and non-strange D mesons is discussed. The second harmonic coefficient provides information about the degree of thermalisation of charm quarks in the medium, while the third one relates to its sensitivity to event-by-event fluctuations in the initial stage of the collision.
A thorough systematic comparison of experimental measurements with phenomenological model calculations will be performed in order to disentangle different model contributions and provide important constraints to the charm-quark diffusion coefficient $D_s$ in the QGP.

Presentation materials

QM22_LVermunt.pdf