Dielectron production in proton-proton and proton-lead collisions at √sNN=5.02TeV

1 shows the ratio of the charged-particle pseudorapidity density in p–Pb and Pb–Pb collisions to the charged- particle pseudorapidity density in pp collisions, all at the

& Alice Wallenberg Foundation (KAW); Ukraine Ministry of Educa- tion and Science; United Kingdom Science and Technology Facili- ties Council (STFC); The United States

Figure 8(c) superimposes the open charm and beauty production measurements re- ported in this paper showing the average prompt D-meson results in the 2 < p T < 4

[2] ALICE Collaboration, Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at √ s = 13 TeV, arXiv:1805.04407[hep-ex].

As there are three different triggers available for the EMCal and hybrid PCM-EMCal methods, and two different ones for the PHOS measurement, each with its own statistical

However, the new measurements of (anti-) 3 He in pp and p–Pb collisions show that also in this case the ratio with respect to the proton production increases as a

The B 3 values for the measurements in pp, p-Pb, and Pb-Pb [11,12] collisions are shown as a function of the mean charged-particle multiplicity density.. In addition,

Left panel: Dielectron invariant mass spectrum from Pb-Pb collisions at √ s NN = 2.76 TeV compared to a hadronic cocktail plus the contribution from thermal radiation and