A hot, dense medium called a quark gluon plasma (QGP) is created in ultrarelativistic heavy
ion collisions. Early in the collision, hard parton scatterings generate high momentum …

Abstract The Nuclotron-based Ion Collider fAcility (NICA) is under construction at the Joint
Institute for Nuclear Research (JINR), with commissioning of the facility expected in late …

At sufficiently high temperature and energy density, nuclear matter undergoes a transition to
a phase in which quarks and gluons are not confined: the quark–gluon plasma (QGP). Such …

The production rates and the transverse momentum distribution of strange hadrons at mid-
rapidity (\(\left| y\right|< 0.5\)) are measured in proton-proton collisions at\(\sqrt {s}\)= 13 TeV …

The production of Ξ− and Ω− baryons and their anti-particles in Pb–Pb collisions at s NN=
2.76 TeV has been measured using the ALICE detector. The transverse momentum spectra …

The yields of the K*(892) 0 and ϕ (1020) resonances are measured in Pb-Pb collisions at s
NN= 2.76 TeV through their hadronic decays using the ALICE detector. The measurements …

The multi-strange baryon yields in Pbsingle bondPb collisions have been shown to exhibit
an enhancement relative to pp reactions. In this work, Ξ and Ω production rates have been …

Abstract General-purpose Monte Carlo event generators have become important tools in
particle physics, allowing the simulation of exclusive hadronic final states. In this article we …

Identified charged-particle spectra of π±, K±, p, and p¯ at midrapidity (| y|< 0. 1) measured by
the dE/dx method in the STAR (solenoidal tracker at the BNL Relativistic Heavy Ion Collider) …

This review aims at providing an extensive discussion of modern constraints relevant for
dense and hot strongly interacting matter. It includes theoretical first-principle results from …