2020
DOI: 10.48550/arxiv.2002.00631
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NA61/SHINE shining more light on the onset of deconfinement

Maciej P. Lewicki,
Ludwik Turko
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Cited by 3 publications
(4 citation statements)
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“…Status of experimental results on energy dependence of the K + /π + ratio at midrapidity in high-energy nuclear collisions. In addition to the previously shown results on central heavy-ion collisions [16][17][18][19][20][21][22][23][24][25][26] and inelastic p+p [19,[27][28][29][30][31] interactions, results on central Be+Be [46], C+C [47,48], Si+Al [49], Si+Si [47,48], Ar+Sc (preliminary) [50,51], Ni+Ni [52,53] and Xe+Xe [54] (right) as a function of a mean number of wounded nucleons, W , in inelastic p+p interactions [27] and central Be+Be [46], C+C [47], Si+Si [47], Ar+Sc (preliminary) [50,51], Au+Au [22], Pb+Pb [16,17] collisions. Experimental results were compared with the PHSD [12,13] (open crosses) and SMASH [14,15] (open circles) predictions.…”
Section: Collisions Of Intermediate-mass Nucleimentioning
confidence: 79%
See 1 more Smart Citation
“…Status of experimental results on energy dependence of the K + /π + ratio at midrapidity in high-energy nuclear collisions. In addition to the previously shown results on central heavy-ion collisions [16][17][18][19][20][21][22][23][24][25][26] and inelastic p+p [19,[27][28][29][30][31] interactions, results on central Be+Be [46], C+C [47,48], Si+Al [49], Si+Si [47,48], Ar+Sc (preliminary) [50,51], Ni+Ni [52,53] and Xe+Xe [54] (right) as a function of a mean number of wounded nucleons, W , in inelastic p+p interactions [27] and central Be+Be [46], C+C [47], Si+Si [47], Ar+Sc (preliminary) [50,51], Au+Au [22], Pb+Pb [16,17] collisions. Experimental results were compared with the PHSD [12,13] (open crosses) and SMASH [14,15] (open circles) predictions.…”
Section: Collisions Of Intermediate-mass Nucleimentioning
confidence: 79%
“…Status of experimental results on energy dependence of the K + /π + ratio at midrapidity in high-energy nuclear collisions. In addition to the previously shown results on central heavy-ion collisions[16][17][18][19][20][21][22][23][24][25][26] and inelastic p+p[19,[27][28][29][30][31] interactions, results on central Be+Be[46], C+C[47,48], Si+Al[49], Si+Si[47,48], Ar+Sc (preliminary)[50,51], Ni+Ni[52,53] and Xe+Xe[54] collisions are shown. Points presenting Pb+Pb/Au+Au and p+p are plotted in pale colours to emphasize intermediate-mass nuclei results.…”
mentioning
confidence: 79%
“…The application of lQCD to the study of such a matter is limited due to the so-called sign problem. However, there are current and future accelerator facilities, such as RHIC [14], Super Proton Synchrotron (SPS) [15,16], Nuclotron-based Ion Collider (NICA) [17], and the Facility for Anti-proton Ion Research (FAIR) [18,19], which have carried out or plan to conduct diverse experimental programs to explore this part of the QCD phase diagram. The sequence of events in relativistic heavy ion collisions involving the generation of hot and dense matter can be outlined as follows: a pre-equilibrium phase, the attainment of thermal (or chemical) equilibrium among partons, the potential formation of Quark-Gluon Plasma (QGP) or a mixed state of QGP and hadron gas, the emergence of a gas comprising hot interacting hadrons, and, ultimately, a freezeout state where the produced hadrons cease strong interactions.…”
Section: Introductionmentioning
confidence: 99%
“…This is a consequence of the fact that after the deconfinement transition occurs in the system, the strangeness yield becomes independent of the collision energy [7][8][9][10]. Recent investigations showed that the K + /π + peak strongly depends on the volume of the system and tends to be less pronounced in small-sized systems [7,11].…”
Section: Introductionmentioning
confidence: 99%