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Longitudinal Flow and Onset of Deconfinement. Marcus Bleicher Institut für Theoretische Physik Goethe Universität Frankfurt Germany. Outline of the talk. Introduction Fluctuations Evidence for mixing Rapidity widths + Landau softest point Summary. The tool: UrQMD v2.2.
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Longitudinal Flow and Onset of Deconfinement Marcus Bleicher Institut für Theoretische Physik Goethe Universität Frankfurt Germany Marcus Bleicher, Florence 2006
Outline of the talk • Introduction • Fluctuations Evidence for mixing • Rapidity widths + Landau softest point • Summary Marcus Bleicher, Florence 2006
The tool: UrQMDv2.2 • Non-equilibrium transport model • Hadrons and resonances • String excitation and fragmentation • Cross sections are parameterized via AQM or calculated by detailed balance • pQCD hard scattering at high energies • Generates full space-time dynamics of hadrons and strings Marcus Bleicher, Florence 2006
Thanks to the UrQMD group@ Frankfurt • Sascha Vogel (Resonances) • Stephane Haussler (Event-by-Event Fluctuations) • Hannah Petersen (Flow at FAIR) • Diana Schumacher (Di-Leptons) • Qingfeng Li (Isospin Dynamics & HBT) • Xianglei Zhu (Elliptic Flow and Charm) • Mohamed Abdel-Aziz (Event-by-Event Fluctuations) • Elena Bratkovskaya (HSD) • and Horst Stoecker (keeping it running) Marcus Bleicher, Florence 2006
Motivation At RHIC: look for signals of freely moving partons.At FAIR/SPS:look for the mixed phase and the onset of deconfinement E. Bratkovskaya, M.Bleicher. et al., PRC 2005 Marcus Bleicher, Florence 2006
Excitation functions: ratios • ‘Horn’ in the ratio not reproduced • well reproduced • relative strange baryon enhancement reproduced E. Bratkovskaya, M.Bleicher. et al., PRC 2005 Marcus Bleicher, Florence 2006
Fluctuation studies • K/p fluctuations increase towards lower beam energy • Significant enhancement over hadronic cascade model • p/p fluctuations are negative • indicates a strong contribution from resonance decays Taken from Christoph Roland NA49 Preliminary NA49 Preliminary Marcus Bleicher, Florence 2006
Energy dependence • Qualitative description OK • Importance of potentials at low energies • Lack of pressure shows up at SPS energies • EoS <-> Flow H. Petersen, X. Zhu, M.B. Marcus Bleicher, Florence 2006
‘Partonic’ dof already atlow SPS energy • Breakdown of v2 in model coincides with onset of ‘partonic’ matter signals onset of change of EoS in the early stage 30 AGeV H. Petersen, X. Zhu, M.B. Marcus Bleicher, Florence 2006
Stopping power UrQMD vs data Pb+Pb/Au+Au • Linear increase of rapidity shift at low energies • ‘Saturation’ above highest SPS energy • However, relative momentum loss is energy independent Marcus Bleicher, Florence 2006
Multiplicities • Temperatures • Elliptic Flow • Correlations have already been studied Can we learn more from the longitudinal dynamics? Marcus Bleicher, Florence 2006
Multiplicity fluctuations Pb+Pb (158 AGeV) in the NA49 acceptance (1.1<yCM<2.9) Extraction of the multiplicity distribution for every NparNote: Calculation is narrower than the data for Npar~45 Marcus Bleicher, Florence 2006
Multiplicity fluctuations at SPS:The problem • The fluctuation is quantified with the • scaled variance : • Enhanced fluctuations for mid- • peripheral collisions are observed Similar results from HIJING, HSD and RQMD Note : - for a poisson distribution, w=1 Marcus Bleicher, Florence 2006
Where is the problem? Pb+Pb (158 AGeV) in the NA49 acceptance (1.1<yCM<2.9) • Mean value correctly reproduced • Variance reproduced for central and very peripheral events • Failure for mid-peripheral events Marcus Bleicher, Florence 2006
Analysis of different windows • the normalized variance : • flat in the projectile hemisphere • larger in the mirror acceptance • even larger in 4p • maximum around Np=40 Konchakovski, Haussler,…, PRC 73 (2006) Marcus Bleicher, Florence 2006
Fluctutions in target region • the fluctuation has a maximum • around Np=25 • introduces an asymetry between • projectile and target participants • leads to an increase of the multiplicity • fluctuation in the target hemisphere Marcus Bleicher, Florence 2006
Correlation length in rapidity • Rapidity window dependence : • correlation length of the order of 1 • unit of rapidity • target and projectile hemisphere are • independent in hadron-string models Marcus Bleicher, Florence 2006
Mixing and fluctuations • I.e. the trigger condition ‘marks’ projectile and target participants • This allows to study the degree of mixing of the matter produced in HIC • Data suggest strong mixing of hemispheres • Hints to expanding initial fireball in contrast to string dynamics M. Gazdzicki and M. Gorenstein:arXiv:hep-ph/0511058 Marcus Bleicher, Florence 2006
What the fluctuations told us… • Initial fireball of newly produced particles • Fireball seems to expand Landau-like • Leads to strong correlations in rapidity We might use Landau-type hydro to explore the properties of this matter Marcus Bleicher, Florence 2006
Pion rapidity density • Pions rapidity densities are Gaussians at all energies D. Ouerdane, QM04 Marcus Bleicher, Florence 2006
Different particle types • NA49 data yields Gaussian rapidity distributions • Also ALL other experiments report Gaussians for newly produced particles Marcus Bleicher, Florence 2006
Fireball expansion • Assumptions:- applies only to newly produced particles- Lorentz contracted nuclei- simplified Hagedorn gas EoS E. Shuryak, Yad. Fiz. 16 (1972) 395similar to Landau hydroFor more praise on Landau hydro see. P. Steinberg Marcus Bleicher, Florence 2006
Rapidity widths • Rapidity width scales linearly with projectile rapidity M. Bleicher, hep-ph/0509314 Marcus Bleicher, Florence 2006
Speed of sound • Analysis of the rapidity data indicates a softest point at20-30 AGeV beam energy M. Bleicher, hep-ph/0509314 Marcus Bleicher, Florence 2006
Its soft, but… • …is it the mixed phase? • UrQMD also describes the rapidity widths • UrQMD has a soft equation of state Marcus Bleicher, Florence 2006
Summary • Fluctuations indicate strongly mixed initial stage • Assumption of Landau-type hydro allows to extract speed of sound from rapidity widths • Apparent local minimum of sound velocity around 20 – 30 AGeV • Nature of this softest point is unclear Marcus Bleicher, Florence 2006