At energies greater than 1015 eV, cosmic-ray particles can be measured only indirectly by
detecting the extensive showers of secondary particles they create in the Earth's …

The nonadditive entropy S q has been introduced in 1988 focusing on a generalization of
Boltzmann–Gibbs (BG) statistical mechanics. The aim was to cover a (possibly wide) class of …

The construction of a Monte Carlo generator for high energy hadronic and nuclear collisions
is discussed in detail. Interactions are treated in the framework of the Reggeon Field Theory …

The centrality dependence of the charged-particle multiplicity density at midrapidity in Pb-Pb
collisions at s NN= 2.76 TeV is presented. The charged-particle density normalized per …

A measurement is presented of the charged hadron multiplicity in hadronic PbPb collisions,
as a function of pseudorapidity and centrality, at a collision energy of 2.76 TeV per nucleon …

Measurements of primary charged hadron multiplicity distributions are presented for non-
single-diffractive events in proton-proton collisions at centre-of-mass energies of\(\sqrt {s} …

RADIOACTIVITY 134 Xe (2β-); measured recoiling nuclei and electrons, decay energy
spectra using LUX-ZEPLIN (LZ) detector of liquid xenon (LXe), with scintillation and electro …

First measurements of dihadron correlationsfor charged particles are presented for central
PbPb collisions at a nucleon-nucleon center-of-mass energy of 2.76 TeV over a broad range …

Abstract Proton–nucleus (p+ A) collisions have long been recognized as a crucial
component of the physics program with nuclear beams at high energies, in particular for …

The determination of the primary energy and mass of ultra-high-energy cosmic-rays
(UHECR) generating extensive air-showers in the Earth's atmosphere, relies on the detailed …