2018
DOI: 10.1103/physrevc.98.054620
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Cumulants of the baryon number from central Au+Au collision at Elab=1.23 GeV/nucleon reveal the nuclear mean-field potentials

Abstract: Fluctuations of the baryon number in relativistic heavy-ion collisions are a promising observable to explore the structure of the QCD phase diagram. The cumulant ratios in heavy ion collisions at intermediate energies (√ sNN < 7 GeV) have not been studied to date. We investigate the effects of mean field potential and clustering on the cumulant ratios of baryon and proton number distributions in Au+Au collisions at beam energy of 1.23 GeV/nucleon as measured by the HADES Collaboration at GSI. Ultrarelativistic… Show more

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Cited by 12 publications
(5 citation statements)
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“…After t = 10 fm/c, the difference in C 2 /C 1 between UrQMD/m and UrQMD/c was negligible and their values approached unity because the particle density was close to zero. The effect of the mean-field potential on the cumulant of particles in the coordinate space was consistent with our previous works [40][41][42]. We checked that the behavior of net baryons was very similar to that of net protons, therefore in the following only the results of the net protons are displayed.…”
Section: A Results In Coordinate Spacesupporting
confidence: 90%
“…After t = 10 fm/c, the difference in C 2 /C 1 between UrQMD/m and UrQMD/c was negligible and their values approached unity because the particle density was close to zero. The effect of the mean-field potential on the cumulant of particles in the coordinate space was consistent with our previous works [40][41][42]. We checked that the behavior of net baryons was very similar to that of net protons, therefore in the following only the results of the net protons are displayed.…”
Section: A Results In Coordinate Spacesupporting
confidence: 90%
“…The present results suggest that heavy-ion collisions mostly probe regions where the nuclear matter liquid-vapor critical point dominates -hence, the observed baryon fluctuations are largely due to remnants of the nuclear liquid-vapor phase transition. This had been suggested also in previous works [43,18,44,45,46,47]. The CP associated with the chiral symmetry restoration in the CMF model lies at µ B ≈ 1.5 GeV and T ≈ 20 MeV.…”
Section: Probing the Phase Diagram By Heavy Ion Collisionssupporting
confidence: 79%
“…These background contributions may arise from the limited detector acceptance/efficiency, initial volume fluctuation, autocorrelation and centrality resolution, centrality width, baryon number conservation, and resonance decay. Some of these effects have been studied previously [35][36][37][38][39][40][41][42][43][44] but remain to be understood properly before solid physics conclusions can be attained.…”
Section: Introductionmentioning
confidence: 99%