Collectivity in a Parton Cascade Zhe Xu BNL, April 30, 2008 with A. El, O. Fochler, C. Greiner and H. Stöcker.

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Presentation transcript:

Collectivity in a Parton Cascade Zhe Xu BNL, April 30, 2008 with A. El, O. Fochler, C. Greiner and H. Stöcker

Zhe Xu Fast Thermalization from pQCD: 2-3 important Equilibr. time: 1 fm/c Elliptic flow v 2 : high in 2-3 Viscosity: small ~ 0.08 Hard probe: R AA ~ 0.1 collisional 2-2 vs. radiational 2-3 energy loss Motivation and Summary P.Huovinen et al., PLB 503, 58 (2001)

Zhe Xu Outline Transport model Results from simulations Analytical calculations

Zhe Xu BAMPS: B oltzmann A pproach of M ulti P arton S catterings A transport algorithm solving the Boltzmann-Equations for on-shell partons with pQCD interactions new development ggg gg (Z)MPC, VNI/BMS, AMPT Elastic scatterings are ineffective in thermalization ! Inelastic interactions are needed ! Transport Model

Zhe Xu Old collision algorithm BUT, difficult to 3  2 ! collision criterion: (ZPC, MPC, VNI/BMS, AMPT)

Zhe Xu Stochastic algorithm P.Danielewicz, G.F.Bertsch, Nucl. Phys. A 533, 712(1991) A.Lang et al., J. Comp. Phys. 106, 391(1993) 3x3x collision rate per unit phase space for incoming particles p 1 and p 2 with  3 p 1 and  3 p 2 : collision probability (Monte Carlo) Space has to be divided into small cells !

Zhe Xu Z. Xu and C. Greiner, PRC 71, (2005) Interaction Probability

Zhe Xu J.F.Gunion, G.F.Bertsch, PRD 25, 746(1982) T.S.Biro at el., PRC 48, 1275 (1993) S.M.Wong, NPA 607, 442 (1996) screened partonic interactions in leading order pQCD screening mass: LPM suppression : the formation time  g : mean free path Gluons freeze out at local energy density = 1 GeV/fm 3.

Zhe Xu Results from the parton cascade BAMPS thermalization transverse energy elliptic flow shear viscosity jet quenching

Zhe Xu : thermalization! Hydrodynamic behavior! 2-2: NO thermalization simulation pQCD simulation pQCD, only 2-2 at collision center: x T <1.5 fm,  z < 0.4 t fm of a central Au+Au at s 1/2 =200 GeV Initial conditions: minijets p T >1.4 GeV; coupling  s =0.3 p T spectra

Zhe Xu A,El, ZX and C.Greiner, arXiv: [hep-ph], published in NPA ggg gg ! This 3-2 is missing in the Bottom-Up scenario (Baier et al.). Initial conditions: Color Glass Condensate Q s =3 GeV; coupling  s =0.3 p T spectra

Zhe Xu time scale of thermalization  = time scale of kinetic equilibration. Theoretical Result !

Zhe Xu total transverse energy per rapidity at midrapidity y=0

Zhe Xu Rapidity dependence of total transverse energy

Zhe Xu Elliptic Flow and Shear Viscosity in 2-3 at RHIC 2-3 Parton cascade BAMPS ZX, Greiner, Stöcker, arXiv: [nucl-th] viscous hydro. Romatschke, PRL 99, ,2007  /s at RHIC > 0.08

Zhe Xu Rapidity Dependence of v 2 : Importance of 2-3! BAMPS ZX,G,S

Zhe Xu first realistic 3d results on jet-quenching with BAMPS dE/dx, static medium (T = 400 MeV) R AA ~ 0.1 cf. S. Wicks et al. Nucl.Phys.A784, 426 nuclear modification factor central (b=0 fm) Au-Au at 200 AGeV O. Fochler

Zhe Xu Inelastic pQCD interactions (23+32) explain: Fast Thermalization Large Collective Flow Small shear Viscosity of QCD matter at RHIC Part of energy loss (for very high energy parton collisional energy loss due to 2-2 dominates.) Initial conditions, hadronization and afterburning determine how imperfect the QGP at RHIC & LHC can be.

Zhe Xu Analytical Calculations for a Gluon Gas

Zhe Xu J.F.Gunion, G.F.Bertsch, PRD 25, 746(1982) T.S.Biro at el., PRC 48, 1275 (1993) S.M.Wong, NPA 607, 442 (1996) screened partonic interactions in leading order pQCD screening mass: LPM suppression : the formation time  g : mean free path

Zhe Xu Cross section does not determine  ! Collision Rate

Zhe Xu gg  gg: small-angle scatterings gg  ggg: large-angle bremsstrahlung distribution of collision angles at RHIC energies

Zhe Xu BUT, this is not the full story !

Zhe Xu Transport Rates ZX and C. Greiner, PRC 76, (2007) Transport rate is the correct quantity describing kinetic equilibration. Transport collision rates have an indirect relationship to the collision-angle distribution. assume

Zhe Xu Transport Rates Large Effect of gg->ggg !

Zhe Xu due to the fact that a 2->3 process brings one more particle toward isotropy than a gg->gg process.

Zhe Xu From Navier-Stokes approximation From Boltzmann-Eq. relation between  and R tr Shear Viscosity 

Zhe Xu Ratio of shear viscosity to entropy density in 2-3 AdS/CFT RHIC ZX and C.Greiner, arXiv: [nucl-th], to be published in PRL.

Zhe Xu Elliptic Flow and Shear Viscosity in 2-3 at RHIC 2-3 Parton cascade BAMPS ZX, Greiner, Stöcker, arXiv: [nucl-th] viscous hydro. Romatschke, PRL 99, ,2007  /s at RHIC > 0.08

Zhe Xu Inelastic pQCD interactions ( ) explain: Fast Thermalization Large Collective Flow Small shear Viscosity of QCD matter at RHIC Part of energy loss (for very high energy parton collisional energy loss due to 2-2 dominates.) Initial conditions, hadronization and afterburning determine how imperfect the QGP at RHIC & LHC can be. Conclusion

Zhe Xu Collective Flow v 2,v 4,v 6 (Zhe Xu) Jet Quenching (Oliver Fochler) Mach Cone (Ioannis Bouras) Dependence on initial conditions (Luan Cheng) Transport coefficients (Felix Reining) Parton Cascade vs. Viscous Hydrodynamics (Andrej El) Hadronization and afterburning (Petersen, Burau, Xu) HBT Ridge Quarks, Heavy Quarks, Direct Photon Entropy production LHC predictions Many body interactions: 3  3, 2  4,... Including fields, coherent effects (Björn Schenke, Xu) Outlook

Zhe Xu

Initial conditions in heavy ion collisions Glauber-type: Woods-Saxon profile, binary nucleon-nucleon collision for a central Au+Au collision at RHIC at 200 AGeV using p 0 =1.4 GeV minijets production with p t > p 0

Zhe Xu The drift term is large. gg  ggg interactions are essential for kinetic equilibration!