Zi-Wei LinCollective flow and QGP properties11/19/2003 ● Why x-t correlation may be important for HBT ● Origin of a large&positive x-t correlation: partonic?

Slides:



Advertisements
Similar presentations
Zi-Wei Lin (ECU) 28th WWND, Puerto Rico April 10, Update of Initial Conditions in A Multiple Phase Transport (AMPT) Model Zi-Wei Lin Department.
Advertisements

Marcus Bleicher, Berkeley, Oct Elliptic Flow in High Energetic Nuclear Collisions Marcus Bleicher & Xianglei Zhu FIAS & Institut für Theoretische.
Detailed HBT measurement with respect to Event plane and collision energy in Au+Au collisions Takafumi Niida for the PHENIX Collaboration University of.
Mass ordering of differential elliptic flow and its violation for  mesons Tetsufumi Hirano Dept. of Physics, The Univ. of Tokyo Matsumoto, Feb ,
1 Heavy Ion Collisions at LHC in a Multiphase Transport Model  A multi-phase transport (AMPT) model  Rapidity and transverse momentum distributions 
Phase transition of hadronic matter in a non-equilibrium approach Graduate Days, Frankfurt, , Hannah Petersen, Universität Frankfurt.
First Results From a Hydro + Boltzmann Hybrid Approach DPG-Tagung, Darmstadt, , Hannah Petersen, Universität Frankfurt.
Forward-Backward Correlations in Relativistic Heavy Ion Collisions Aaron Swindell, Morehouse College REU 2006: Cyclotron Institute, Texas A&M University.
CERN May Heavy Ion Collisions at the LHC Last Call for Predictions Initial conditions and space-time scales in relativistic heavy ion collisions.
Forward-Backward Correlations in Heavy Ion Collisions Aaron Swindell, Morehouse College REU Cyclotron 2006, Texas A&M University Advisor: Dr. Che-Ming.
1 Systematic studies of freeze-out source size in relativistic heavy-ion collisions by RHIC-PHENIX Akitomo Enokizono Lawrence Livermore National Laboratory.
1 Isotropization of an equilibrating Quark-Gluon Plasma Bin Zhang a, Lie-Wen Chen b, Che-Ming Ko c a Arkansas State University, b Shanghai Jiaotong University,
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.
Resonance Dynamics in Heavy Ion Collisions 22nd Winter Workshop on Nuclear Dynamics , La Jolla, California Sascha Vogel, Marcus Bleicher UrQMD.
Collision system dependence of 3-D Gaussian source size measured by RHIC-PHENIX Akitomo Enokizono Lawrence Livermore National Laboratory 23 rd Winter Workshop.
1 Searching for the QGP at RHIC Che-Ming Ko Texas A&M University  Signatures of QGP  Quark coalescence Baryon/meson ratio Hadron elliptic flows and quark.
Marcus Bleicher, CCAST- Workshop 2004 Strangeness Dynamics and Transverse Pressure in HIC Marcus Bleicher Institut für Theoretische Physik Goethe Universität.
Sept WPCF-2008 Initial conditions and space-time scales in relativistic heavy ion collisions Yu. Sinyukov, BITP, Kiev Based on: Yu.S., I. Karpenko,
Uncertainties in jet event generators due to hadronizaton scheme, Other issues with energy loss on E-by-E hydro, and the extraction of transport coefficients.
Narrowing of Balance Function and Hadronization Time at RHIC Energy Du Jiaxin, and Liu Lianshou Institute Of Particle Physics, Huazhong Normal University.
Identified Particle Ratios at large p T in Au+Au collisions at  s NN = 200 GeV Matthew A. C. Lamont for the STAR Collaboration - Talk Outline - Physics.
KROMĚŘĺŽ, August 2005WPCF Evolution of observables in hydro- and kinetic models of A+A collisions Yu. Sinyukov, BITP, Kiev.
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.
Longitudinal de-correlation of anisotropic flow in Pb+Pb collisions Victor Roy ITP Goethe University Frankfurt In collaboration with L-G Pang, G-Y Qin,
Richard Lednický Femtoscopic search for the 1-st order PT Femtoscopic signature of QGP 1-st order PT Solving Femtoscopy Puzzle.
Jaipur February 2008 Quark Matter 2008 Initial conditions and space-time scales in relativistic heavy ion collisions Yu. Sinyukov, BITP, Kiev (with participation.
Marcus Bleicher, TBS Berkeley 2005 What have we learned from transport models? Marcus Bleicher Institut für Theoretische Physik Goethe Universität Frankfurt.
1 Tatsuya Chujo Univ. of Tsukuba Soft particle production at RHIC CNS-RIKEN workshop “Physics of QGP at RHIC” (Feb. 16, 2006)
Hadron emission source functions measured by PHENIX Workshop on Particle Correlations and Fluctuations The University of Tokyo, Hongo, Japan, September.
Anisotropic flow, Azimuthal Balance Function, and Two-charged-particle Azimuthal Correlations in RQMD and AMPT We are very grateful to Zhixu Liu and Jiaxin.
1 Jeffery T. Mitchell – Quark Matter /17/12 The RHIC Beam Energy Scan Program: Results from the PHENIX Experiment Jeffery T. Mitchell Brookhaven.
LP. Csernai, NWE'2001, Bergen1 Part II Relativistic Hydrodynamics For Modeling Ultra-Relativistic Heavy Ion Reactions.
Flow fluctuation and event plane correlation from E-by-E Hydrodynamics and Transport Model Victor Roy Central China Normal University, Wuhan, China Collaborators.
XXXI Max Born Symposium and HIC for FAIR Workshop, Wrocław June 15, 20131/31 Recent Developments of A Multi-Phase Transport Model Zi-Wei Lin Department.
Sergey Panitkin Current Status of the RHIC HBT Puzzle Sergey Panitkin Brookhaven National Lab La Thuile, March 18, 2005.
Masashi Kaneta, First joint Meeting of the Nuclear Physics Divisions of APS and JPS 1 / Masashi Kaneta LBNL
July 22, 2004R. Soltz, Hot Quarks, Taos, NM1 Future Directions in HBT This title has been used before These predictions are seldom right Title.
In Medium Hadronization: Hadrons and Jets Rainer Fries Texas A&M University Jet Modifications in the RHIC and LHC Era Wayne State, August 20, 2014 With.
Azimuthal HBT measurement of charged pions With respect to 3 rd event plane In Au+Au 200GeV collisions at RHIC-PHENIX Takafumi Niida for the PHENIX Collaboration.
1 Transport description of viscous effects Che-Ming Ko Texas A&M University  Introduction  A multi-phase transport (AMPT) model  Anisotropic flow -
1 June 24-29, Levoca, Slovakia Baryon-strangeness correlations in a partonic/hadron transport model F. Jin, Y. G. Ma, X. Z. Cai, G. L. Ma, H. Huang,
Heavy-Ion Physics - Hydrodynamic Approach Introduction Hydrodynamic aspect Observables explained Recombination model Summary 전남대 이강석 HIM
School of Collective Dynamics in High-Energy CollisionsLevente Molnar, Purdue University 1 Effect of resonance decays on the extracted kinetic freeze-out.
HBT two-pion correlations at LHC Qingfeng Li ( 李庆峰 ) (Huzhou Teachers College)
R. Lednicky: Joint Institute for Nuclear Research, Dubna, Russia I.P. Lokhtin, A.M. Snigirev, L.V. Malinina: Moscow State University, Institute of Nuclear.
Scott PrattMichigan State University Femtoscopy: Theory ____________________________________________________ Scott Pratt, Michigan State University.
Budapest, 4-9 August 2005Quark Matter 2005 HBT search for new states of matter in A+A collisions Yu. Sinyukov, BITP, Kiev Based on the paper S.V. Akkelin,
1 Che-Ming Ko Texas A&M University  QCD phase diagram  Signatures of QGP  Experimental observations at RHIC and theoretical interpretations  RHIC low.
Jin-Hui Chen Shanghai Institute of Applied Physics, CAS In collaboration with F. Jin, D. Gangadharan, X. Cai, H. Huang and Y. Ma Parton distributions at.
Charm elliptic flow at RHIC B. Zhang 1, L.W. Chen 2, C.M. Ko 3 1 Arkansas State University, 2 Shanghai Jiao Tong University, 3 Texas A&M University Charm.
Understanding the rapidity dependence of v 2 and HBT at RHIC M. Csanád (Eötvös University, Budapest) WPCF 2005 August 15-17, Kromeriz.
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.
Elliptic flow and incomplete equilibration in AMPT Jian-Li Liu Harbin Institute of Technology.
Elliptic Anisotropy v2 May Be Dominated by Particle Escape Zi-Wei Lin (with L He, T Edmonds, F Liu, D Molnar, FQ Wang) Quark Matter /17 Elliptic.
JET Collaboration Meeting June 17-18, 2014, UC-Davis1/25 Flow and “Temperature” of the Parton Phase from AMPT Zi-Wei Lin Department of Physics East Carolina.
1 Space-time analysis of reactions at RHIC Fabrice Retière Lawrence Berkeley Lab STAR collaboration.
Japanese Physics Society meeting, Hokkaido Univ. 23/Sep/2007, JPS meeting, Sapporo, JapanShinIchi Esumi, Inst. of Physics, Univ. of Tsukuba1 Collective.
Global and Collective Dynamics at PHENIX Takafumi Niida for the PHENIX Collaboration University of Tsukuba “Heavy Ion collisions in the LHC era” in Quy.
Shear Viscosity and Collective Flow in Heavy Ion Collisions within Parton Cascade Calculations Zhe Xu, Carsten Greiner Trento, Sept. 17, 2009 Institut.
SQM2003March 13Zi-wei Lin The Ohio State University ● Why transport model? ● Space-time (x-t) correlation: its effect on R out/ R side Extract radii from.
Adam Kisiel – CERN Hirschegg 2010 – 19 Jan Femtoscopy in relativistic heavy-ion collisions as a probe of system collectivity Adam Kisiel CERN.
Hydro + Cascade Model at RHIC
Heavy-Flavour Physics in Heavy-Ion Collisions
Experimental Studies of Quark Gluon Plasma at RHIC
Introduction Results Methods Conclusions
Institute of Particle Physics Huazhong Normal University
Effect of equilibrium phase transition on multiphase transport in relativistic heavy ion collisions 喻 梅 凌 华中师范大学粒子物理研究所 2019/2/24 第十届全国粒子物理大会 桂林.
Two Particle Interferometry at RHIC
Presentation transcript:

Zi-Wei LinCollective flow and QGP properties11/19/2003 ● Why x-t correlation may be important for HBT ● Origin of a large&positive x-t correlation: partonic? resonance decays? hadronic rescatterings? ● Can a (hydro-type) negative x-t correlation survive decays/rescatterings in a transport model? Rout/Rside: from Gaussian fit vs from emission function Strong and positive x-t correlation and its effect on Rout/Rside Zi-Wei Lin The Ohio State University

Zi-Wei LinCollective flow and QGP properties11/19/2003 HBT Radii from Emission function S(x,p) or correlation function C(q) If source is Gaussian in space-time, then: Rsource,ij=Rfit,ij 1) Curvature at q=0: 2) Often use 4-parameter fit for C(q) w/o Coulomb effects: Pratt,PRL84 Wiedemann,PRC57 Dx,y= -. 2

Zi-Wei LinCollective flow and QGP properties11/19/2003 Study HBT with a transport model Advantage: freezeout in transport is natural as the mean free path grows too big compared with system size How to relate to hydro calculations (Cooper-Frye formula at a sharp hypersurface is usually imposed)

Zi-Wei LinCollective flow and QGP properties11/19/2003 HIJING energy in strings and minijet partons ZPC (Zhang's Parton Cascade) Till Parton freezeout ART (A Relativistic Transport model for hadrons) A+A Decay all resonances; Final particle spectra Structure of AMPT model with String Melting Fragment excited strings into partons Coalescence into hadrons

Zi-Wei LinCollective flow and QGP properties11/19/2003 ZWL,Ko&Pal,PRL89 From Gaussian fits to 3-d correlation function C(q) Au+Au at 130AGeV (b=0 fm)

Zi-Wei LinCollective flow and QGP properties11/19/2003 Why x-t correlation may be important? Spatial-size x-t correlationduration-time Magnitude and sign of x-t correlation are important for Rout, Rout/Rside, & extraction of duration-time

Zi-Wei LinCollective flow and QGP properties11/19/2003 Correlations in pion emission source: out-side out-t Positive and large, tends to reduce Rout Values: (17fm)**2 = * Source Spatial-size x-t correlationDuration time ZWL,Ko&Pal,PRL89 Note:includes  decays

Zi-Wei LinCollective flow and QGP properties11/19/2003 out-side out-t K emission source (excludes  decays): ZWL&Ko,JPG29 Values: (3.4fm)**2 = 35 -2* K source also positive and large for K

Zi-Wei LinCollective flow and QGP properties11/19/2003 ● Turn off  decays to study HBT radii from the emission function ● Test hydro-like negative x-t correlation upon hadron formation in AMPT

Zi-Wei LinCollective flow and QGP properties11/19/2003 Pions at freezeout x out x side x y mostly partons ~surface emission ~volume emission >0 parton transverse flow

Zi-Wei LinCollective flow and QGP properties11/19/2003 x-t correlation for pions Au+Au at 200AGeV (b=0 fm)

Zi-Wei LinCollective flow and QGP properties11/19/2003 Already present for quarks x-t correlation for pions Au+Au at 200AGeV (b=0 fm)

Zi-Wei LinCollective flow and QGP properties11/19/2003 Effect of decays on source radii Hadronic decays produce mt-dependence in Rout & Rside

Zi-Wei LinCollective flow and QGP properties11/19/2003 Rout/Rside from emission function

Zi-Wei LinCollective flow and QGP properties11/19/2003 Can an initial negative x-t correlation survive later? Test negative x-t correlation from hydro models at RHIC energies

Zi-Wei LinCollective flow and QGP properties11/19/2003 large initial Rout/Rside ratio (source) Initial hadrons:

Zi-Wei LinCollective flow and QGP properties11/19/2003 large final Rout/Rside ratio (source) Negative x-t term becomes positive after hadronic scatterings Final hadrons:

Zi-Wei LinCollective flow and QGP properties11/19/2003 Hardtke&Voloshin, PRC61 Radii are different from source or from Gaussian fit to C(Q)

Zi-Wei LinCollective flow and QGP properties11/19/2003 from source from C(Q) fit big decrease for fitted Rout, Rout/Rside AMPT: Au+Au at 200AGeV at b=0 fm, 3mb Rout/Rside=1

Zi-Wei LinCollective flow and QGP properties11/19/2003 from source from C(Q) fit With an initial negative x-t correlation at hadron formation huge decrease for fitted Rout & Rout/Rside Rout/Rside >>1~=1 Rout/Rside=1

Zi-Wei LinCollective flow and QGP properties11/19/2003 ● Strong and positive x out -t correlation term ● tends to reduce R out and R out /R side. ● already present at parton freezeout/hadron formation ● An initial negative x-t correlation can lead to large R out /R side (when evaluated from emission function) ● R out /R side: >1 from emission function ~=1 from Gaussian fits to C(Q). ● Even with an large initial negative x-t (with Rout/Rside >>1 from the emission function) ● Further investigation is needed to find the reason. HBT summary