LP. Csernai, Sept. 4, 2001, Palaiseau FR 1 L.P. Csernai, C. Anderlik, V. Magas, D. Strottman.

Slides:

Advertisements

Similar presentations

Multi-strange Hadron v2 and Partonic Collectivity

Advertisements

Further development of the HydroKinetic Model (hHKM) and description of the RHIC and LHC A+A data Yu. M. Sinyukov Bogolyubov Institute for Theoretical.

PID v2 and v4 from Au+Au Collisions at √sNN = 200 GeV at RHIC

Photon Physics with PHOS

Mass, Quark-number, Energy Dependence of v 2 and v 4 in Relativistic Nucleus- Nucleus Collisions Yan Lu University of Science and Technology of China Many.

R. Lacey, SUNY Stony Brook 1 Arkadij Taranenko Quark Matter 2006 November 13-20, Shanghai, China Nuclear Chemistry Group SUNY Stony Brook, USA PHENIX Studies.

New Results from Viscous Hydro + URQMD (VISHNU) International School for High Energy Nuclear Collisions, Wuhan, Oct 31- Nov.5, 2011 References: Supported.

R. Lacey, SUNY Stony Brook 1 Arkadij Taranenko Helmholtz International Summer School: “Dense Matter In Heavy Ion Collisions and Astrophysics” Dubna, Russia,

What do we Learn From Azimuthal Correlation Measurements in PHENIX Roy. A. Lacey Nuclear Chemistry, SUNY, Stony Brook.

Marcus Bleicher, Berkeley, Oct Elliptic Flow in High Energetic Nuclear Collisions Marcus Bleicher & Xianglei Zhu FIAS & Institut für Theoretische.

Elliptic flow of thermal photons in Au+Au collisions at 200GeV QNP2009 Beijing, Sep , 2009 F.M. Liu Central China Normal University, China T. Hirano.

Duke University Chiho NONAKA in Collaboration with Masayuki Asakawa (Kyoto University) Hydrodynamical Evolution near the QCD Critical End Point June 26,

1 Transport and Hydrodynamic Model for Ultra-relativistic Heavy Ion Collisions Yu-Liang Yan China Institute of Atomic Energy Collaborators: Yun Cheng (CCNU,

LP. Csernai, Montreal Topics in Heavy Ion Collisions, 2003 Montreal, June 25-28, 2003 Flow effects and their measurable consequences in ultra-relativistic.

L.P. Csernai 1 Freeze-out and constituent quark formation in a space-time layer.

Norway. 3-dim. QGP Fluid Dynamics and Flow Observables László Csernai (Bergen Computational Physics Lab., Univ. of Bergen)

CERN May Heavy Ion Collisions at the LHC Last Call for Predictions Initial conditions and space-time scales in relativistic heavy ion collisions.

DNP03, Tucson, Oct 29, Kai Schweda Lawrence Berkeley National Laboratory for the STAR collaboration Hadron Yields, Hadrochemistry, and Hadronization.

Terence Tarnowsky Long-Range Multiplicity Correlations in Au+Au at Terence J Tarnowsky Purdue University for the STAR Collaboration 22nd Winter Workshop.

Nu XuInternational Conference on Strangeness in Quark Matter, UCLA, March , 20061/20 Search for Partonic EoS in High-Energy Nuclear Collisions Nu.

Freeze-Out in a Hybrid Model Freeze-out Workshop, Goethe-Universität Frankfurt Hannah Petersen.

Marcus Bleicher, WWND 2008 A fully integrated (3+1) dimensional Hydro + Boltzmann Hybrid Approach Marcus Bleicher Institut für Theoretische Physik Goethe.

Properties of the Quantum Fluid at RHIC Strangeness in Quark Matter March 26-31, 2006.

DPG spring meeting, Tübingen, March Kai Schweda Lawrence Berkeley National Laboratory for the STAR collaboration Recent results from STAR at RHIC.

The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences Cracow, Poland Based on paper M.Ch., W. Florkowski nucl-th/ Characteristic.

Sept WPCF-2008 Initial conditions and space-time scales in relativistic heavy ion collisions Yu. Sinyukov, BITP, Kiev Based on: Yu.S., I. Karpenko,

Particle Spectra at AGS, SPS and RHIC Dieter Röhrich Fysisk institutt, Universitetet i Bergen Similarities and differences Rapidity distributions –net.

Flow Vorticity and Rotation in Peripheral HIC Dujuan Wang CBCOS, Wuhan, 11/05/2014 University of Bergen, Norway.

Perfect Fluid: flow measurements are described by ideal hydro Problem: all fluids have some viscosity -- can we measure it? I. Radial flow fluctuations:

Flow fluctuation and event plane correlation from E-by-E Hydrodynamics and Transport Model LongGang Pang 1, Victor Roy 1,, Guang-You Qin 1, & Xin-Nian.

Two particle correlation method to Detect rotation in HIC Dujuan Wang University of Bergen Supervisor: Laszlo P. Csernai.

LP. Csernai, PASI'2002, Brazil1 Part I Relativistic Hydrodynamics For Modeling Ultra-Relativistic Heavy Ion Reactions.

L.P. Csernai 1 Laszlo P. Csernai, University of Bergen, Norway Differential HBT method to detect rotation Wigner - CCNU mini Workshop, Budapest, Apr. 7-8,

Scaling properties of multiplicity fluctuations in heavy-ion collisions simulated by AMPT model Yi-Long Xie China University of Geosciences, Wuhan （ Xie.

Jaipur February 2008 Quark Matter 2008 Initial conditions and space-time scales in relativistic heavy ion collisions Yu. Sinyukov, BITP, Kiev (with participation.

Norway Relativistic Hydrodynamics and Freeze-out László Csernai (Bergen Computational Physics Lab., Univ. of Bergen)

Anisotropic flow, Azimuthal Balance Function, and Two-charged-particle Azimuthal Correlations in RQMD and AMPT We are very grateful to Zhixu Liu and Jiaxin.

Energy Dependence of ϕ -meson Production and Elliptic Flow in Au+Au Collisions at STAR Md. Nasim (for the STAR collaboration) NISER, Bhubaneswar, India.

LP. Csernai, NWE'2001, Bergen1 Part II Relativistic Hydrodynamics For Modeling Ultra-Relativistic Heavy Ion Reactions.

L.P. Csernai, BNL Nov '03 1 L..P. Csernai Multi module modelling of heavy ion collisions Collective flow and QGP properties RIKEN-BNL workshop November.

Flow fluctuation and event plane correlation from E-by-E Hydrodynamics and Transport Model Victor Roy Central China Normal University, Wuhan, China Collaborators.

CCAST, Beijing, China, 2004 Nu Xu //Talk/2004/07USTC04/NXU_USTC_8July04// 1 / 26 Collective Expansion in Relativistic Heavy Ion Collisions -- Search for.

LP. Csernai, NWE'2001, Bergen1 Part III Relativistic Hydrodynamics For Modeling Ultra-Relativistic Heavy Ion Reactions.

PHOTONS AND EVOLUTION OF A CHEMICALLY EQUILIBRATING AND EXPANDING QGP AT FINITE BARYON DENSITY Shanghai Institute of Applied Physics Jiali Long, Zejun.

Results from an Integrated Boltzmann+Hydrodynamics Approach WPCF 2008, Krakau, Jan Steinheimer-Froschauer, Universität Frankfurt.

Two freeze-out model for the hadrons produced in the Relativistic Heavy-Ion Collisions. New Frontiers in QCD 28 Oct, 2011, Yonsei Univ., Seoul, Korea Suk.

S. PrattNSCL/MSU Deciphering the Space-Time Evolution of Heavy-Ion Collisons with Correlation Measurements Scott Pratt Michigan State University.

Roy A. Lacey, Stony Brook, ISMD, Kromĕříž, Roy A. Lacey What do we learn from Correlation measurements at RHIC.

Characterization of the pion source at the AGS Mike Lisa The Ohio State University Motivation and Measurement Systematics of HBT in E895 Existing problems.

Andras. Ster, RMKI, Hungary ZIMANYI-SCHOOL’09, Budapest, 01/12/ Azimuthally Sensitive Buda-Lund Hydrodynamic Model and Fits to Spectra, Elliptic.

Particle emission in hydrodynamic picture of ultra-relativistic heavy ion collisions Yu. Karpenko Bogolyubov Institute for Theoretical Physics and Kiev.

Helen Caines Yale University Strasbourg - May 2006 Strangeness and entropy.

Fluctuations, Instabilities and Collective Dynamics L. P. Csernai 1 and H. Stöcker 2 1 Institute of Physics and Technology, University of Bergen, Allegaten.

Elliptic flow from initial states of fast nuclei. A.B. Kaidalov ITEP, Moscow (based on papers with K.Boreskov and O.Kancheli) K.Boreskov and O.Kancheli)

ISMD 2016 August 29, 2016 Jeju island, South Korea

Experiment Review in small system collectivity and thermalization in pp, pA/dA/HeA collisions Shengli Huang.

Directed flow of identified particles from Au+Au Collisions at RHIC

Directed Flow of Identified Particles

CCNU-UiB-CIAE Workshop, May 2011 中国—挪威研讨会， 2011年 5月

Initial States and Global Dynamics versus Fluctuations

Hydro + Cascade Model at RHIC

Collective Dynamics at RHIC

Directed Flow Measurements at STAR

Effects of Bulk Viscosity on pT Spectra and Elliptic Flow Coefficients

QGP in small colliding systems?

Differential HBT method to detect rotation

System Size and Energy Dependence of -meson Production at RHIC

Norwegian High-Energy Heavy Ion Theory

Strong Magnetic Fields in HIC

Dipartimento Interateneo di Fisica, Bari (Italy)

Presentation transcript:

LP. Csernai, Sept. 4, 2001, Palaiseau FR 1 L.P. Csernai, C. Anderlik, V. Magas, D. Strottman

LP. Csernai, Sept. 4, 2001, Palaiseau FR 2 Multi Module Modeling Initial state - pre-equilibrium: Parton Cascade; Coherent Yang-Mills [Magas] Local Equilibrium  Hydro, EoS Final Freeze-out: Kinetic models, measurables If QGP  Sudden and simultaneous hadronization and freeze out (indicated by HBT, Strangeness, Entropy puzzle) Landau (1953), Milekhin (1958), Cooper & Frye (1974)

LP. Csernai, Sept. 4, 2001, Palaiseau FR 3 Matching Conditions  Conservation laws  Nondecreasing entropy

LP. Csernai, Sept. 4, 2001, Palaiseau FR 4 INITIAL STATE

LP. Csernai, Sept. 4, 2001, Palaiseau FR 5

6 Firestreak Picture Myers, Gosset, Kapusta, Westfall

LP. Csernai, Sept. 4, 2001, Palaiseau FR 7 String rope --- Flux tube --- Coherent YM field

LP. Csernai, Sept. 4, 2001, Palaiseau FR 8 Initial stage: Coherent Yang-Mills model [Magas, Csernai, Strottman, NEW’2001]

LP. Csernai, Sept. 4, 2001, Palaiseau FR 9 Yo – Yo Dynamics

LP. Csernai, Sept. 4, 2001, Palaiseau FR 10

LP. Csernai, Sept. 4, 2001, Palaiseau FR 11 Expanding string ropes – Full energy conservation

LP. Csernai, Sept. 4, 2001, Palaiseau FR 12 Initial state 3 rd flow component

LP. Csernai, Sept. 4, 2001, Palaiseau FR 13 3-Dim Hydro for RHIC (PIC)

LP. Csernai, Sept. 4, 2001, Palaiseau FR 14 3-dim Hydro for RHIC Energies Au+Au E CM =65 GeV/nucl. b=0.1 b max A σ =0.08 => σ~10 GeV/fm n / n 0 [ 1 ] e [ GeV / fm 3 ] T= 0.0 fm/c n max = 8.67 e max =32.46 GeV / fm 3 L x,y = 1.45 fm L z =0.145 fm x 1.3 fm

LP. Csernai, Sept. 4, 2001, Palaiseau FR 15 3-dim Hydro for RHIC Energies Au+Au E CM =65 GeV/nucl. b=0.1 b max A σ =0.08 => σ~10 GeV/fm n / n 0 [ 1 ] e [ GeV / fm 3 ] T=1.9 fm/c n max = 8.66 e max = GeV / fm 3 L x,y = 1.45 fm L z =0.145 fm..

LP. Csernai, Sept. 4, 2001, Palaiseau FR 16 3-dim Hydro for RHIC Energies Au+Au E CM =65 GeV/nucl. b=0.1 b max A σ =0.08 => σ~10 GeV/fm n / n 0 [ 1 ] e [ GeV / fm 3 ] T= 3.8 fm/c n max = 7.77 e max = GeV / fm 3 L x,y = 1.45 fm L z =0.145 fm x 1.3 fm

LP. Csernai, Sept. 4, 2001, Palaiseau FR 17 3-dim Hydro for RHIC Energies Au+Au E CM =65 GeV/nucl. b=0.1 b max A σ =0.08 => σ~10 GeV/fm n / n 0 [ 1 ] e [ GeV / fm 3 ] T= 5.7 fm/c n max = 6.36 e max = GeV / fm 3 L x,y = 1.45 fm L z =0.145 fm..

LP. Csernai, Sept. 4, 2001, Palaiseau FR 18 3-dim Hydro for RHIC Energies Au+Au E CM =65 GeV/nucl. b=0.1 b max A σ =0.08 => σ~10 GeV/fm n / n 0 [ 1 ] e [ GeV / fm 3 ] T= 7.6 fm/c n max = 5.22 e max = GeV / fm 3 L x,y = 1.45 fm L z =0.145 fm..

LP. Csernai, Sept. 4, 2001, Palaiseau FR 19 3-dim Hydro for RHIC Energies Au+Au E CM =65 GeV/nucl. b=0.1 b max A σ =0.08 => σ~10 GeV/fm n / n 0 [ 1 ] e [ GeV / fm 3 ] T= 9.5 fm/c n max = 4.45 e max = GeV / fm 3 L x,y = 1.45 fm L z =0.145 fm..

LP. Csernai, Sept. 4, 2001, Palaiseau FR 20 Global Flow Directed Transverse flow Elliptic flow 3 rd flow component (anti - flow) 3 rd flow component (anti - flow) Squeeze out

LP. Csernai, Sept. 4, 2001, Palaiseau FR 21 Third flow component [SPS NA49]

LP. Csernai, Sept. 4, 2001, Palaiseau FR 22 Third flow component / SPS / NA49

LP. Csernai, Sept. 4, 2001, Palaiseau FR 23 3 rd flow component and QGP Csernai & Röhrich [Phys.Lett.B458(99)454] observed a 3 rd flow component at SPS energies, not discussed before. Also observed that in ALL earlier fluid dynamical calculations with QGP in the EoS there is 3 rd flow comp. The effect was absent without QGP. In string and RQMD models only peripheral collision showed the effect (shadowing). The effect is attributed to a flat (Landau type) initial condition. Similarity to elliptic flow.

LP. Csernai, Sept. 4, 2001, Palaiseau FR 24 3 rd flow component Hydro [Csernai, HIPAGS’93]

LP. Csernai, Sept. 4, 2001, Palaiseau FR 25 A= fm / c

LP. Csernai, Sept. 4, 2001, Palaiseau FR 26 A= fm/c

LP. Csernai, Sept. 4, 2001, Palaiseau FR 27 Freeze out

LP. Csernai, Sept. 4, 2001, Palaiseau FR 28 Hypersurface

LP. Csernai, Sept. 4, 2001, Palaiseau FR 29 “Cooper-Frye” formula

LP. Csernai, Sept. 4, 2001, Palaiseau FR 30 Consequences of conservation laws:  Non-decreasing entropy current across front! (Space-like [Taub 1948], Time-like [Csernai 1987])

LP. Csernai, Sept. 4, 2001, Palaiseau FR 31 Space-like hypersurface

LP. Csernai, Sept. 4, 2001, Palaiseau FR 32 Cut – Juttner distribution: Pre FO velocity [Anderlik et al., Phys.Rev.C59(99)3309] [Bugaev, Nucl.Phys.A606(96)559] Θ(p.dσ) f(x,p)

LP. Csernai, Sept. 4, 2001, Palaiseau FR 33 Kinetic freeze-out models  Kinetic approach  f (x,p) out of equilibrium  Asymmetry

LP. Csernai, Sept. 4, 2001, Palaiseau FR 34 Freeze out model with rescattering [Anderlik et al., Phys.Rev.C59: ,1999 ]

LP. Csernai, Sept. 4, 2001, Palaiseau FR 35 Freeze out distribution with rescattering V=0 [V. Magas, et al.,] Heavy Ion Phys.9: ,1999

LP. Csernai, Sept. 4, 2001, Palaiseau FR 36 P-t distribution (T=130 MeV) [V. Magas et al., Phys.Lett.B459(99)33]

LP. Csernai, Sept. 4, 2001, Palaiseau FR 37