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The Physics of Compressed Nuclear Matter at GSI and FAIR The 10th International Conference on Nucleus-Nucleus Collisions, August 16-21, 2009, Beijing, China Joachim Stroth, Goethe-University / GSI, Germany
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Agenda o Motivation o Recent remarkable results from SIS18 o The persepective and challenge at FAIR o Summary Not included in the talk – Bulk observables, Fluctuations, Flow
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The phase diagram of nuclear matter Chemical freeze-out points derived from Statistical Hadronization Model Universal conditions for freeze-out (?) Limiting temperature T max ? Why is it woking at low beam energies? QCD inspired models demonstrate the melting of the condesates. A. Andronic, P. Braun-Munzinger, K. Redlich, J. Stachel J. Cleymans, K. Redlich LQCD explores unknown regions from solid grounds at B =0. T c = T max ? 1st order phase transition Critical point ? Schäfer, Wambach priv. communication Schäfer, Wambach priv. communication Leupold J.Phys.G32:2199,2006 LHC RHIC SPS FAIR SIS AGS
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Ignorant interpretation (Cloudy Bag Model) q q q q q q q q q q q q q q q q q q q q q q q q 1 fm : equiv. to 100 MeV (uncertainty relation)
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T T c, m B ~ 0 q q q q q q q q q q q q q q q q q q q q q q q q qq - - - - - - - - - Excitation/melting of the vacuum/cloud. smooth cross over
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T << T c, finite B q q q q q q q q q q q q q q q q q q q q q q q q qq -
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T << T c, finite B q q q q q q q q q q q q q q q q q q q q q q q q Bag fusion mixed phase
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Phase diagram from large N c limit McLerran, Pisarski: QM09 conjecture for N c = 3 Quarkyonic Matter: Confined gas of perturbative quarks!
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Strange Particle Production at SIS18 HADES, Ar+KCl at 1.76 GeV/u FOPI (P. Gasik CPOD 2009), Al+Al at 2 GeV/u T chem = 70 3 MeV B = 746 15 MeV R C = 2.6 0.4 fm preliminary Statistical Model: THERMUS, S. Wheaton and J. Cleymans, hep-ph/0407174 Transport: UrQMD, M. Bleicher, S. Vogel at al. HADES collab.: arXiv:0907.3582 HADES collab.: arXiv:0907.3582 and arXiv:0902.3487arXiv:0902.3487
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Properties of the Fireball at below E beam < 30 GeV/u Long lifetime of the high- density phase Baryon dominated Extented region of a strongly interacting hadron gas Red line from Hadron Gas Model, Sasaki QM09
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Dileptons from 1 and 2 GeV/u 12 C+ 12 C runs Phys.Rev. Lett 98(2007) 052302 Phys. Lett. B 663 (2008) 43 Good normalization established in 0 region Measured pair excess in C+C scales with beam energy as production What is the contribution from the initial phase? l+l+ l-l- ** ** l+l+ l-l- ** l+l+ l-l-
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12 Electron-pair spectrum decomposition Mesons (known) Baryon resonances Not measured but important at lower beam energies Two-body decays (known) : e+ e- e+ e- e+ e- pp @3.5 GeV 00 //
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The solution to the DLS puzzle C+C collisions compared to NN reference HADES data agrees with DLS
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Electron pairs from Ar+KCl at 1.76 GeV/u First observation of mesons in HI collisions at these energies x 2 PLUTO A Compared to reference after subtraction of contributions from preliminary F ~ 3
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The Future at GSI and FAIR SIS18 Several FOPI runs on strangeness production in 2008 – 2010 Upgraded HADES (20 KHz reaction rate) Au+Au and Ag+Ag, pion induced reactions from 2010 on. SIS100: Joint running of HADES and preCBM, multistrange particle and lepton pair excitation function, charm production in proton induced reactions SIS300: Full exploitation of rare probes a high B; fluctuations, flow
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Particle multiplicities in detection channel Au+Au at 25 GeV/u HSD transport calculation and statistical hadronization model. Not fully dressed in HI collisions at AGS and lower SPS energies
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The Quest for the Highest Densities J. Randrup and J. Cleymans, hep-ph/0607065 Freeze-out configurations for X+X collisions in the net-baryon density and energy density plane.
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Low-mass vector mesons. What do they tell about chiral symmtery restoration?
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Low-mass lepton pairs, … the link to the microscopic properties of dense baryonic matter … the link to the microscopic properties of dense baryonic matter. Special role of the meson: – short life time – „photon-like“ – coupling to baryons! isentropic expansion Thermal dilepton rates see e.g. R. Rapp, J. Wambach and H. Hees : arXiv:0901.3289, and S. Leupold, U. Mosel and V. Metag arXiv:0907.2388 R.Arnaldi,etal.[NA60collaboration], Phys.Rev.Lett.96,162302(2006 R.Arnaldi,etal.[NA60collaboration], Phys.Rev.Lett.96,162302(2006 )
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New approaches in theory Hybrid codes for modeling the reaction dynamics 1.Non-equilibrium initial conditions via UrQMD 2.Hydrodynamic evolution or Transport calculation 3.Freeze-out via adronic cascade (UrQMD) hydro running time hydro start time Pb+Pb, central (Petersen et al., PRC 78:044901, 2008, arXiv: 0806.1695) Introduce virtual photon emissivity from in-medium spectral functions with hydro codes R. Rapp, H. van Hees, V. Toneev, J. Wambach, B. Friman, Texas A&M, TU Darmstadt, GSI, Giessen, Frankfurt
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Ring Imaging Cherenkov Detector Transition Radiation Detectors Electron identification in CBM
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Electron-pair reconstruction in CBM Challenge -No electron identification before tracking -Background due to material budget of the STS -Sufficient discrimination (600 /event misidentification 10 -4 ) Reduction of background by reconstructing pairs from -conversion (~3 ) and Dalitz decay (8 /event) e-e- e+e+ 00 00 Track Segment Track Fragment
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Background rejection performance Central Au+Au collisions at 25 GeV/u Free cocktail only (without medium contribution) Statistic: 200000 events = beam spill on target All e + e - Combinatorial bg Invariant mass spectrum after all cuts applied Invariant mass spectrum identified e + e -
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M ll > 200 MeV/c 2 safety factor ;) NA60 In+In @ 158 AGeV CERES Pb+Au @ 40 AGeV CERES Pb+Au @ 158 AGeV (σ/σ tot = 28%) CERES Pb+Au @ 158 AGeV (σ/σ tot = 7%) CERES Pb+Au @ 158 AGeV PHENIX Au+Au @ √s = 200 AGeV Comparison of expected performance to existing dilepton experiments
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Charmonium suppression. c c -
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The Charm of CBM Rare but measurement feasible! – Very sparse experimental information – At threshold, production mechanism in pA and AA unclear. Open charm in CBM BRM / 10 12 events 1) 4 10 -5 56000 1 10 -4 174000 9 10 -5 195000 4 10 -5 103000 10 12 events 40 weeks running at 10 5 interaction rate. Event selection: Real-time vertex finding in 20 Gbyte data/s. W. Cassing, E.L. Bratkovskaya, and A. Sibirtsev, Nucl.Phys.A691,753(2001)
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Near threshold charm production < 20 MeV~ 780 MeV760 MeV97 % ~ 190 MeV1020 MeV830 MeV81 % ~ 2500 MeV3097 MeV597 MeV19 % Does charm at FAIR play the same role like Strangeness at GSI? Substantial differences due to the large charm quark masses: – Different interaction/production mechanism (Meson vs. Pomeron exchange) – Charm pair produced in very short instant of time (~ 1/m c, i.e. of order 0,1 fm) – Hadron formation time possibly similar (time needed to establish the proper sea- quark and gluon distribution) Medium-effects may determine the charm distribution over hadronic degrees of freedeom but likely not the multiplicity!
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Charm propagation How are the produced charm quarks propagating in the dense phase, quark like or (pre-)hadron like ? – Charmonium over open charm as indicator! – Charmed baryons important for a complete picture. – Are there indications of collectivity. O. Linnyk, E. Bratkovskaya and W. Cassing, arXiv:0808.1504v1 A. Andronic, P. Braun-Munzinger, et al., Phys. Lett. B 659 (2007) 149, arXiv:0708.1488
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Summary – „Long-lived“ states of dense nuclear matter are produced in collisions of heavy ion at energies of a few GeV/u. – The phase in the high-density region might be much more exotic then a hadron/resonance gas. – Unfortunately, there is no smoking gun, but: Fast equillibration „Sub-threshold“ production Strong broadening of in-medium states – Close collaboration with, and novel approaches in theory are necessary to make the case.
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