Azimuthally-differential femtoscopic measurements, being sensitive to spatio-temporal characteristics of the source as well as to the collective velocity fields at freeze out, provide very important information on the ...

Results on the production of stable light nuclei, including deuterons,3He,4He and the corresponding anti-nuclei, inPb–Pb collisions at√sNN=2.76 TeV and√sNN=5.02 TeV are presented and compared with theoretical predictionsand ...

ALICE is the experiment specifically designed to study the Quark-Gluon Plasma (QGP) in heavy-ion collisions at the CERN LHC. The ALICE detector will be upgraded during the Long Shutdown 2, planned for 2019-2020, in order ...

One of the key results of the LHC Run 1 was the observation of an enhanced production of strange particles in high multiplicity pp and p–Pb collisions at √ sNN = 7 and 5.02 TeV, respectively. The strangeness enhancement ...

Quarkonia, i.e. bound states of bb¯ and cc¯ quarks, are powerful observables to study the properties of nuclear matter under extreme conditions. The formation of a Quark-Gluon Plasma (QGP), which is predicted by lattice ...

Measurements of open heavy flavour production in p–A collisions allow the investigation of Cold Nuclear Matter effects. In addition, they are an important tool for a complementary investigation of the long-range correlations ...

Femtoscopic correlations between charged pions and kaons for different charge combinations are measured in Pb−Pb collisions at √ sNN = 2.76 TeV with ALICE at the LHC. The three-dimensional pion-kaon (π − K) correlation ...

We present recent results on strange and non-strange D-meson production measured with ALICE in Pb–Pb collisions at the LHC. In addition, the measurements of the Λ+ c -baryon production and of the Λ+ c /D0 ratio in pp, p–Pb, ...

The production of muons from heavy-flavour hadron decays in p–Pb collisions at was studied for GeV/c with the ALICE detector at the CERN LHC. The measurement was performed at forward (p-going direction) and backward ...

The second and the third order anisotropic flow, V2 and V3, are determined by the corresponding initial spatial anisotropy coefficients, ε2 and ε3, in the initial density distribution. On the contrary, the higher order ...