Relativistic p+ A collisions may produce droplets of quark-gluon plasma (QGP) that quickly
develop a toroidal vortex structure similar to that of an expanding smoke ring. We present …

The production of Z 0 bosons at large rapidities in Pb–Pb collisions at s NN= 5.02 TeV is
reported. Z 0 candidates are reconstructed in the dimuon decay channel (Z 0→ μ+ μ−) …

A bstract Inclusive J/ψ yields and average transverse momenta in p-Pb collisions at a center-
of-mass energy per nucleon pair\(\sqrt {s_ {\mathrm {NN}}}\)= 8. 16 TeV are measured as a …

Angular correlations between heavy-flavor decay electrons and charged particles at
midrapidity (| η|< 0.8) are measured in p-Pb collisions at s NN= 5.02 TeV. The analysis is …

In ultrarelativistic heavy-ion experiments, one estimates the centrality of a collision by using
a single observable, say n, typically given by the transverse energy or the number of tracks …

The measurement of the azimuthal-correlation function of prompt D mesons with charged
particles in pp collisions at\(\sqrt {s}= 5.02\\hbox {TeV}\) and p–Pb collisions at\(\sqrt {s …

The dependence of f0 (980) production on the final-state charged-particle multiplicity in p–
Pb collisions at√ 𝑠NN= 5.02 TeV is reported. The production of f0 (980) is measured with …

This paper is a write-up of the ideas that were presented, developed and discussed at the
third International Workshop on QCD Challenges from pp to A–A, which took place in August …

Charged jet production cross sections in p–Pb collisions at s NN= 5.02 TeV measured with
the ALICE detector at the LHC are presented. Using the anti-k T algorithm, jets have been …

Abstract The two Zero Degree Calorimeters (ZDCs) of the CMS experiment are located
at±140 m from the collision point and detect neutral particles in the| η|> 8.3 pseudorapidity …