QCD Plasma Thermalization and Collective Flow Effects Zhe Xu CCAST, Beijing, March 23, 2008.

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Presentation transcript:

QCD Plasma Thermalization and Collective Flow Effects Zhe Xu CCAST, Beijing, March 23, 2008

Zhe Xu Y X Fast Thermalization from QCD: 3-2 important Equilibr. time: short in 2-3 Elliptic flow v 2 : high in 2-3 Viscosity: small ~ 0.08 Three body effects in parton cascades! P.Huovinen et al., PLB 503, 58 (2001) from R. Bellwied

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 ! Xiong, Shuryak, PRC 49, 2203 (1994) Dumitru, Gyulassy, PLB 494, 215 (2000) Serreau, Schiff, JHEP 0111, 039 (2001) Baier, Mueller, Schiff, Son, PLB 502, 51 (2001)

Zhe Xu Stochastic algorithm Z. Xu and C. Greiner, PRC 71, (2005) for particles in  3 x with momentum p 1,p 2,p 3... interaction probability: cell configuration in space 3x3x

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

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 Cross section does not determine  ! ZX and C.Greiner, arXiv: [nucl-th] What determines the equilibration time scale  ?

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.

Zhe Xu Transport Rates Large Effect of 2-3 !

Zhe Xu Shear Viscosity  D.Teaney, PRC 68, (2003) P.Arnold, G.D.Moore, L.G.Yaffe, JHEP 0011, 001 (2001); 0305, 051 (2003) T.Hirano, M.Gyulassy, NPA 769, 71 (2006) M.Asakawa, S.A.Bass, B.Müller, Prog.Theor.Phys. 116, 725 (2007) A.Muronga, PRC 76, (2007) ZX, C.Greiner, arXiv: [nucl-th]

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

Zhe Xu Ratio of shear viscosity to entropy density in 2-3 AdS/CFT RHIC

Zhe Xu Collective Effects

Zhe Xu total transverse energy per rapidity at midrapidity

Zhe Xu transverse flow velocity of local cell in the transverse plane of central rapidity bin Au+Au b=8.6 fm using BAMPS =c

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 see also: L.W.Chen, et al., PLB 605, 95 (2005) C.Nonaka, et al., JPG 31, 429 (2005) T.Hirano, et al., PLB 636, 299 (2006) J.Bleibel, et al., PRC 76, (2007); PLB 659, 520 (2008) Hama, et al., arXiv: [hep-ph] A.K.Chaudhuri, arXiv:

Zhe Xu Inelastic pQCD interactions ( ) explain: Fast Thermalization Large Collective Flow Small shear Viscosity of QCD matter at RHIC Initial conditions, hadronization and afterburning determine how imperfect the QGP at RHIC & LHC can be. Summary

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

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

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

Zhe Xu Thermalization driven by plasma instabilities Refs.: Mrowczynski; Arnold, Lenaghan, Moore, Yaffe; Rebhan, Romatschke, Strickland; Bödeker, Rummukainen; Dumitru, Nara; Berges, Scheffler, Sexty. Dumitru, Nara, Strickland, PRD 75, (2007) Dumitru, Nara, Schenke, Strickland, arXiv:

Zhe Xu QCD thermalization using parton cascade VNI/BMS: K.Geiger and B.Müller, NPB 369, 600 (1992) S.A.Bass, B.Müller and D.K.Srivastava, PLB 551, 277(2003) ZPC: B. Zhang, Comput. Phys.Commun. 109, 193 (1998) MPC: D.Molnar and M.Gyulassy, PRC 62, (2000) AMPT: B. Zhang, C.M. Ko, B.A. Li, and Z.W. Lin, PRC 61, (2000) BAMPS: Z. Xu and C. Greiner, PRC 71, (2005); 76, (2007)

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)

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