Dynamical Modeling of Relativistic Heavy Ion Collisions Tetsufumi Hirano hirano_at_phys.s.u-tokyo.ac.jp Collaborators:

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Presentation transcript:

Dynamical Modeling of Relativistic Heavy Ion Collisions Tetsufumi Hirano hirano_at_phys.s.u-tokyo.ac.jp Collaborators: M.Gyulassy, Y.Nara, U.Heinz, D.Kharzeev, R.Lacey, T.Gunji, H.Hamagaki, T.Hatsuda, M.Isse, A.Ohnishi, K.Yoshino, R.Mizukawa

Outline Introduction Dynamical modeling of heavy ion collisions Bulk Hard/rare probes and interplay btw. soft and hard Summary and Outlook

Phase Diagram of QCD Taken from Understanding of phase diagram and EOS is one of the main topics in modern nuclear physics.

Constraint of EOS from Observation of Compact Stars Mass-Radius relation Model EOS Tolman-Oppenheimer-Volkov eq. : Pressure as a function of mass-energy density Taken from Lattimer, Prakash(’06) Observation of compact star mass (Hydrostatic equilibrium) TOV eq. plays an important role in understanding of EOS Taken from Lattimer, Prakash(’06)

Phase Diagram of QCD Taken from

Constraint of Cosmological Parameters from CMB Observation COBE, WMAP,… Taken from “Best” cosmological parameters C.L.Bennett et al.,Ap.J.Suppl(’03) CMB tools: CMBFAST, CAMB, … CMB tools: CMBFAST, CAMB, … Analysis codes play a major role in precision physics.

Phase Diagram of QCD Taken from

Complexity Non-linear interactions of gluons Strong coupling Dynamical many body system Color confinement Inputs to phenomenology (lattice QCD) “Mind The Gap” The first principle (QuantumChromo Dynamics) Experimental Relativistic Heavy Ion Collider ~150 papers from 4 collaborations since 2000 Phenomenology (hydrodynamics) ex.)QCDOC

Lessons from Other Fields Necessity of collaborative activity in more extended community Necessity of analysis tool(s) in R.H.I.C. physics Toward establishment of the “observational QGP physics” phenomenology people lattice people experimental people

Dynamical Modeling Based on 3D Ideal Hydrodynamics

Current Status of Dynamical Modeling in H.I.C. Proper time Transverse momentum CGC Geometric Scaling Shattering CGC Hydrodynamics viscosityviscosity non chem. eq.non chem. eq. Parton energy loss InelasticInelastic ElasticElastic Hadroniccascade Low p T High p T RecombinationCoalescence “DGLAP region” (N)LOpQCD Before collisions PartonproductionPre-equilibrium “Perfect” fluid QGP or GP Dissipativehadrongas Fragmentation Interaction Intermediate p T fluctuationInstability?Equilibration? T.Hirano and Y.Nara(’02-)

BULK 3D Hydro 3D Hydro+Cascade CGC initial conditions

Centrality Dependence of v 2 Discovery of “large” v 2 at RHIC v 2 data are comparable with hydro results for the first time. Hadronic cascade models cannot reproduce data. This is the first time for ideal hydro at work in H.I.C.  Strong motivation to develop hydro-based tools. Result from a hadronic cascade (JAM) (Courtesy of M.Isse) TH et al. (’06). AuAu200

Pseudorapidity Dependence of v 2 v 2 data are comparable with 3D hydro results again around =0 Not a QGP gas  sQGP Nevertheless, large discrepancy in forward/backward rapidity  See next slides TH(’02); TH and K.Tsuda(’02); TH et al. (’06). QGP only QGP+hadron AuAu200

Importance of Hadronic “Corona” Boltzmann Eq. for hadrons instead of hydrodynamics Including viscosity through finite mean free path Perfect fluid QGP core + Dissipative hadronic corona QGP only QGP+hadron fluids QGP fluid+hadron gas T.Hirano et al.,Phys.Lett.B636(2006)299. T.Hirano and M.Gyulassy,Nucl.Phys.A769 (2006)71. AuAu200

Highlights from a QGP Hydro + Hadronic Cascade Model Works quite well! b=7.2fm 0-50% Adapted from S.J.Sanders QM2006 AuAu200

Sensitivity to Initial Conditions Novel initial conditions from “Color Glass Condensate” lead to large eccentricity. Need viscosity even in QGP! Hirano and Nara(’04), Hirano et al.(’06) Kuhlman et al.(’06), Drescher et al.(’06)

HARD/RARE PROBES Hydro+Jet model Hydro+J/ model Interplay btw. soft and hard Jet-fluid string formation

Utilization of Hydro Results Jet quenching J/psi suppression Meson Recombination Coalescence Thermal radiation (photon/dilepton) Information along a path Information on surface Information inside medium Baryon J/psi c c bar

Jet Propagation through a QGP Fluid Color: parton density Plot: mini-jets Au+Au 200AGeV, b=8 fm transverse Fragmentation switched off hydro+jet model x y Full 3D ideal hydrodynamics + PYTHIA Parton distribution fn. pQCD 2  2 processes Fragmentation Gyulassy-Levai-Vitev formula Inelastic energy loss T.Hirano and Y.Nara (’02-)

p T Distribution from Hydro+Jet Model Soft + Quenched Hard picture works reasonably well  Re/Co components may be needed for a better description Note: Hadronic cascade is switched off in the bulk T.Hirano and Y.Nara, Phys.Rev.C69,034908(2004).

Back-To-Back Correlation T.Hirano and Y.Nara, Phys.Rev.Lett.91,082301(2003). Not only energy loss but also deflection are found to be important.

Melting of J/ in a QGP Fluid T.Gunji et al., hep-ph/ ~hirano/parevo/parevo.html open hydro data table Dynamics is important in understanding onset of suppression  Stay tuned! Talk by T.Gunji, 16:10- Suppression factor of J/

Hadronization through Jet- Fluid String Formation Hirano, Isse, Nara, Ohnishi, Yoshino, Mizukawa, nucl-th/ ; (work in progress) Space-time evolution of the QGP fluid  Open data table String Fragmentation  PYTHIA (Lund) Energy loss  GLV 1 st order

Summary & Outlook Development of an analysis code in H.I.C. QGP fluid + hadronic gas picture works well Sensitivity to initial conditions in hydro EOS dependence (not discussed in this talk) Application of hydro results Single- and di-hadron distributions at high p T J/ suppression Jet-Fluid String formation (EM probes) Toward an open and standard tool in H.I.C. (like PYTHIA, CMBFAST, …)