Multihadron production dynamics exploring the energy balance in hadronic and nuclear collisions
EKG Sarkisyan, AN Mishra, R Sahoo, AS Sakharov - Physical Review D, 2016 - APS
The relation of multihadron production in nucleus-nucleus and (anti) proton-proton collisions
is studied by exploring the collision-energy and centrality dependencies of the charged …
is studied by exploring the collision-energy and centrality dependencies of the charged …
ϒ production in p–Pb collisions at sNN= 8.16 TeV
S Acharya, D Adamová, A Adler, J Adolfsson… - Physics Letters B, 2020 - Elsevier
ϒ production in p–Pb interactions is studied at the centre-of-mass energy per nucleon–
nucleon collision s NN= 8.16 TeV with the ALICE detector at the CERN LHC. The …
nucleon collision s NN= 8.16 TeV with the ALICE detector at the CERN LHC. The …
Diffractive and non-diffractive wounded nucleons and final states in pA collisions
C Bierlich, G Gustafson, L Lönnblad - Journal of High Energy Physics, 2016 - Springer
A bstract We review the state-of-the-art of Glauber-inspired models for estimating the
distribution of the number of participating nucleons in pA and AA collisions. We argue that …
distribution of the number of participating nucleons in pA and AA collisions. We argue that …
System-size dependence of the charged-particle pseudorapidity density at sNN= 5.02 TeV for pp, pPb, and PbPb collisions
S Acharya, D Adamová, A Adler, GA Rinella, M Agnello… - Physics Letters B, 2023 - Elsevier
We present the first systematic comparison of the charged-particle pseudorapidity densities
for three widely different collision systems, pp, psingle bondPb, and Pbsingle bondPb, at the …
for three widely different collision systems, pp, psingle bondPb, and Pbsingle bondPb, at the …
Forward production at high energy: Centrality dependence and mean transverse momentum
B Ducloue, T Lappi, H Mäntysaari - Physical Review D, 2016 - APS
Forward rapidity J/ψ meson production in proton-nucleus collisions can be an important
constraint of descriptions of the small-x nuclear wave function. In an earlier work we studied …
constraint of descriptions of the small-x nuclear wave function. In an earlier work we studied …
Multiplicity and transverse momentum evolution of charge-dependent correlations in pp, p–Pb, and Pb–Pb collisions at the LHC
ALICE Collaboration alice-publications@ cern … - The European Physical …, 2016 - Springer
We report on two-particle charge-dependent correlations in pp, p–Pb, and Pb–Pb collisions
as a function of the pseudorapidity and azimuthal angle difference, Δ η Δ η and Δ φ Δ φ …
as a function of the pseudorapidity and azimuthal angle difference, Δ η Δ η and Δ φ Δ φ …
Charged-particle pseudorapidity density at mid-rapidity in p–Pb collisions at s_ NN s NN= 8.16 TeV
The pseudorapidity density of charged particles, d N_ ch/d η d N ch/d η, in p–Pb collisions
has been measured at a centre-of-mass energy per nucleon–nucleon pair of s_ NN s NN …
has been measured at a centre-of-mass energy per nucleon–nucleon pair of s_ NN s NN …
Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV
ALICE collaboration - arXiv preprint arXiv:1805.05212, 2018 - arxiv.org
Charged-particle spectra at midrapidity are measured in Pb-Pb collisions at the centre-of-
mass energy per nucleon-nucleon pair $\sqrt {s_ {\rm NN}} $= 5.02 TeV and presented in …
mass energy per nucleon-nucleon pair $\sqrt {s_ {\rm NN}} $= 5.02 TeV and presented in …
Prompt and non-prompt production and nuclear modification at mid-rapidity in p–Pb collisions at TeV
S Acharya, FT Acosta, D Adamová, J Adolfsson… - The European Physical …, 2018 - Springer
A measurement of beauty hadron production at mid-rapidity in proton-lead collisions at a
nucleon–nucleon centre-of-mass energy s_ NN= 5.02 s NN= 5.02 TeV is presented. The …
nucleon–nucleon centre-of-mass energy s_ NN= 5.02 s NN= 5.02 TeV is presented. The …
[HTML][HTML] Production of and in p–Pb collisions at TeV
D Adamová, MM Aggarwal, G Aglieri Rinella… - The European Physical …, 2017 - Springer
The transverse momentum distributions of the strange and double-strange hyperon
resonances (\(\Sigma (1385)^{\pm}\),\(\Xi (1530)^{0}\)) produced in p–Pb collisions at\(\sqrt …
resonances (\(\Sigma (1385)^{\pm}\),\(\Xi (1530)^{0}\)) produced in p–Pb collisions at\(\sqrt …