International School on: Quark-Gluon Plasma and Heavy Ion Collisions: Past, Present, Future Villa Gualino, Turino, Italy Soft Probes II Christoph Blume University of Heidelberg Observables Temperature Strangeness Resonances Femtoscopy Fluctuations Flow Jets + Heavy Flavor Photons Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Strangeness Strangeness in Heavy Ion Physics Strangeness enhancement as a QGP signature J. Rafelski and B. Müller, PRL48, 1066 (1982) P. Koch, B. Müller, and J. Rafelski, Phys. Rep. 142, 167 (1986) Strangeness has to be produced (no s-Quarks in nucleons) Thresholds are high in hadronic reactions, e.g..: N + N N + K+ + (Ethres 700 MeV) Fast equilibration in a QGP via partonic processes, e.g. gluon-fusion ⇒ Enhancement of strange particle production in A+A relative to p+p expected (in particular multi-strange particles) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Statistical Models Multiplicities determined by statistical weights (⇒ chemical equilibrium) A.Andronic et al. PLB673, 142 (2009) Grand-canonical partition function: ⇒ Parameters: V, T, μB, γS F.Becattini et al., PRC69, 024905 (2004) Details: see F. Becattini’s lecture Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Hadronic Transport Models Microscopic approach Pb+Pb @ √sNN = 17.3 GeV UrQMD Hadronic degrees of freedom Non-equilibrium Production mechanisms: Measured and parameterized cross sections String-excitation and fragmentation Medium effects, Examples: Multi-meson fusion, UrQMD Mass shifts, HSD ... NEXUS (AMPT) (EPOS) ... Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Strange Particles Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Major Strangeness Carriers: Kaons and Lambdas Strangeness Conservation s Isospin Symmetry Isospin Symmetry K- (us) s = K0 (ds) K+ (us) >> (uds) >> (uds) If baryon density is high Christoph Blume Villa Gualino, Turino, 7-12 March 2011 K0 (ds) Measurement of Charged Kaons via dE/dx Bethe-Bloch function: Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Combination of dE/dx and Time-Of-Flight (TOF) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Weak Decay Topologies V0 Topology (K0s, Λ): Ξ- (Cascade) Ω- Topology: Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Strangeness Production in a Pion-Proton Event p + - - K0 Associated production: - Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Strangeness Production in a Heavy Ion Event Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Reconstruction via Decay Topology NA49 NA57 Christoph Blume NA57 Villa Gualino, Turino, 7-12 March 2011 Armenteros-Podolanski Plot Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Strangeness Enhancement (SPS) NA57: JPG32, 427 (2006) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Strangeness Enhancement (RHIC) STAR: PRC77, 044908 (2008) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Enhancement Towards Lower Energies √sNN (GeV) Contrary to naive expectation Same behavior for multi-strange particles? Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Particle Ratios in p+p: RHIC and LHC Increase of relative strangeness production in p+p with √s ALICE: arXiv:1012.3257 Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Ξ at Threshold Energies Expectation for statistical model (Andronic et al.) HADES: PRL103, 132301 (2009) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Strangeness Enhancement as QGP Signature ? Is it a dominantly partonic effect or can hadronic processes lead to the same fast equilibration? Multi-meson fusion processes C. Greiner and S. Leupold, J. Phys. G 27, L95 (2001) Dynamic equilibration at the phase boundary? P. Braun-Munzinger, J. Stachel, and C. Wetterich, Phys. Lett. B 596, 61 (2004) Hadronization generally a statistical phenomenon? U. Heinz, Nucl. Phys. A 638, 357c (1998), R. Stock, Phys. Lett. B 456, 277 (1999) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Energy Dependence of K/π Ratios Quite sharp maximum in K+/π+ ratio Indication for phase transition (?) PRC77, 024903 (2008) arXiv:1007.2613 Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Energy Dependence of Hyperon/π Ratios |y| < 0.4 / -/ |y| < 0.5 − +/ − / = 1.5 (+ + -) PRC78, 034918 (2008) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Maximum of Relative Strangeness Production Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Chemical Freeze-Out Curve Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Chemical Freeze-Out in the QCD Phase Diagram Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Spectra Rapidity Distributions ... BRAHMS: Au+Au, √sNN = 200 GeV Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Landau ... p+p Data Pion production ~ Entropy Isentropic expansion Description of the pion gas as a 3D relativistic fluid Prediction: dN/dy is Gaussian of a width given by: L. D. Landau, Izv. Akad. Nauk. SSSR 17 (1953) 52 P. Carruthers and M. Duong-Van, PRD8 (1973) 859 Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Landau ... works also for Heavy Ions BRAHMS: PRL94, 162301 (2005) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Width of the Φ Rapidity Distribution Expectation for kaon coalescence K+ + K- → Φ PRC78, 044907 (2008) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 1/mT dN/dmT 1/mT dN/dmT Radial Expansion and Transverse Momentum Spectra mT mT No radial flow: exponential spectrum (p+p collisions) Christoph Blume With radial flow: add. boost by expansion (vT) ⇒ blue shifted spectrum Villa Gualino, Turino, 7-12 March 2011 Blast Wave Analysis of Particle Spectra Central Pb+Pb 158A GeV E. Schnedermann and U. Heinz, PRC50, 1675 (1994) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Energy Dependence of Kinetic Freeze-Out arXiv:1007.2613 Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Energy Dependence of 〈mT〉 NA49: PRC77, 024903 (2008) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Radial Expansion of Strange Particles What about heavy particles (Ξ, Ω, J/ψ) ? NA57: JPG32, 2065 (2006) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Radial Expansion of Strange Particles Particles with low hadronic cross sections: Ξ, Ω, J/ψ ⇒ Not sensitive to flow in hadronic, but maybe to partonic phase N. Xu and M. Kaneta, NPA698, 306 (2002) 306. Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Radial Expansion of Strange Particles Multi-strange particles sensitive to the partonic flow contribution (?) STAR: PRL92, 182301 (2004) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Resonances Resonances Strong decays ⇒ short lifetimes that can be in the order of the fireball lifetime Examples: K(892) → K+ + π - : Φ(1020) → K+ + K- : cτ = 3.91 fm cτ = 46.5 fm Σ-(1385) → Λ + π - : Λ(1520) → p + K- : cτ = 5.08 fm cτ = 12.7 fm Should be sensitive to the late phase of the hadronic fireball Regeneration Rescattering of decay products ⇒ Provide information on the time span between chemical and kinetic freeze-out Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Recombination and Rescattering of Resonances Picture adapted from C. Markert and P. Fachini Hot and dense medium Particle yields Particle spectra K K K* π K* K π π Time Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Measurement of Resonances: Σ(1385) and Λ(1520) STAR: PRC71, 064902 (2005) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Rescattering after Chemical Freeze-Out STAR: PRC71, 064902 (2005) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Comparison to Chemical Equilibrium Expectation Pb+Pb, √sNN = 17.3 GeV Pb+Pb, √sNN = 17.3 GeV NA49: pub. in preparation HGM: F. Becattini et al. Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Scaling Properties of the Φ Meson No scaling with K+ × K(coalescence picture) 2 Scaling _ with (s-Quarks) Φ = ss _ + K ∝ s-Quarks K- + Λ ∝ s-Quarks Christoph Blume Villa Gualino, Turino, 7-12 March 2011 K+/π + and Λ/π – Compared to Statistical Model A. Andronic et al., PLB676, 142 (2009) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Energy Dependence of K/π Ratios Quite sharp maximum in K+/π+ ratio Indication for phase transition (?) PRC77, 024903 (2008) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Antibaryon-Baryon Ratios S = -3 S = -2 S = -1 S=0 NA49: PRC78, 034918 (2008) Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Baryon-Meson-Ratios Baryon-Meson Ratio: Λ/K0s Λ/K0s > 1: Cannot be understood in string fragmentation picture Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Hadronization Mechanisms Fragmentation (Lund model) _ String fragments via qq creation Original parton momentum is divided among resulting partons Quark coalescence Hadrons form by combining quarks from quark soup (QGP) Would be dominating at intermediate pt Christoph Blume Villa Gualino, Turino, 7-12 March 2011 Fragmentation vs Coalescence Hadron from fragmentation: ph = z p, z < 1 Hadron from coalescence: ph = p1 + p2 Production of baryons favored relative to mesons in coalescence picture Christoph Blume Villa Gualino, Turino, 7-12 March 2011 _ Baryon-Meson Ratio: Ω(sss)/Φ(ss) Christoph Blume Villa Gualino, Turino, 7-12 March 2011