A (re)interpretation of the QCD phase transition and of strangeness as QGP signature

dc.creatorKabana, Sonja
dc.date2001-05-15
dc.date.accessioned2026-07-07T03:44:31Z
dc.date.available2026-07-07T03:44:31Z
dc.descriptionThe temperature at the chemical freeze-out and at zero baryochemical potential has been extracted in a global analysis of $e^+e^-$, $p+p$, $p+ \overline{p}$ and $A+A$ collisions at $\sqrt{s}$=2-1800 GeV per N+N pair. We demonstrate that the temperature at $μ_B$=0, rises with the initial energy density $ε_i$, and saturates above $ε_i$ $\sim$ 1 GeV/fm$^3$. This behaviour is interpreted as mapping out the QCD phase transition universally in particle and nuclear collisions. The critical energy density is therefore identified to be $ε_{crit}$ $\sim$ 1 $\pm$ 0.3 GeV/fm$^3$. We show that strange particles at $μ_B$=0, are not significantly enhanced in A+A collisions as compared to $p+ \overline{p}$. The so called 'strangeness suppression factor' ($λ_s = \frac{(2 \overline{s})} {(\overline{u} + \overline{d})}$) as a function of $ε_i$ is following the temperature, rising and saturating universally above $ε_{crit}$. This leads to a reinterpretation of strangeness enhancement as QGP signature. Within this interpretation the experimental puzzles with respect to strangeness production can be naturally explained: e.g. the recent measured maximum of $K^+/π^+$ in Pb+Pb collisions at 40 A GeV, is explained as due to $μ_B$. We discuss under which conditions 'strangeness enhancement' and '$J/Ψ$ suppresion' both set in at $ε_{crit}$ $\sim$ 1 GeV/fm$^3$.
dc.description8 pages, 5 figures, XXXVIth Rencontres de Moriond on 'QCD and high energy hadronic interactions', 17-24 March 2001, Les Arcs 1800, France
dc.identifierhttps://arxiv.org/abs/hep-ph/0105152
dc.identifierhttp://arxiv.org/abs/hep-ph/0105152
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/40594
dc.subjectHigh Energy Physics - Phenomenology
dc.titleA (re)interpretation of the QCD phase transition and of strangeness as QGP signature
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