1. Viscosities and QCD Phase Transitions Jiunn-Wei Chen National Taiwan U.

4. QCD Phase Diagram

5. Elliptic Flow Figure: H. Meyer

6. QGP EOS (LQCD) ~ an ideal gas Karsch hep-lat/0106019

7. Elliptic Flow: QGP ~ a strongly interacting fluid Figure: H. Meyer Luzum, Romatschke, 2008 Photon elliptic flow: see Fu Ming LIU’s talk

8. QGP EOS (LQCD) ~ an ideal gas Karsch hep-lat/0106019

9. Shear viscosity Frictional force

10. Shear viscosity measures how “perfect” a fluid is! Smaller shear viscosity implies larger particle interaction!

11. Kovtun, Son, and Starinets (’05) Conjecture: Shear viscosity / entropy density Motivated by AdS/CFT ( see talks of JUGEAU & YAKHSHIEV, LU & BRODSKY )

13. “QGP” (quark gluon plasma) almost saturates the bound @ just above Tc (Teaney; Romatschke, Romatschke; Song, Heinz ) LQCD, gluon pasma (Karsch, Wyld; Nakamura, Sakai; Meyer) QGP near Tc, a near perfect fluid, SQGP PQGP: Asakawa, Bass, Müller; Xu, Greiner

14. QCD Phase Diagram

15. Pion gas ChPT (chiral perturbation theory) Non-perturbative in coupling Boltzman equation Earlier work: Prakash, Prakash, Venugopalan, Welke; Dobado, Llanes-Estrada; Csernai, Kapusta, McLerran NJL: see Shi Jun Mao’s talk

16. JWC, Nakano

17. QCD Phase Diagram

18. JWC, Li, Liu, Nakano

19. Lacey et al., PRL 98:092301,2007; 2007 US Nuclear Science Long Range Plan Cold Unitary Atoms Rupak & Schafer 2007 Nuclear liquid-gas Phase transition JWC et al. 2007 goes to a local minimum near a phase transition in more than 30 systems with no exception found so far. T 0 /T F

20. 2nd-order p.t.: a 0, c = 0 crossover: + No p.t.: a > 0, b > 0, c = 0 1st-order phase transition a > 0, b 0 (JWC, M. Huang, Y.H. Li, E. Nakana, D.L. Yang)

21. Weak coupling, Boltzmann eq. Mean field calculation CJT formulism (Cornwall, Jackiw, Tomboulis)

22. of Water (Lacey et al.)

23. QCD Bulk Viscosity (Chiral Limit) Karsch, Kharzeev, Tuchin; Meyer; JWC, Wang

24. QCD Bulk Viscosity Karsch, Kharzeev, Tuchin; Meyer; JWC, Wang See also Fernandez-Fraile, Gomez Nicola

25. Bulk Viscosity Li, Huang Gubser, Nellore, Pufu, Rocha

26. Outlook I: Universality? Universal and behaviors? ( reaches local minimum near p.t. reaches local maximum near p.t.)

27. Mapping QCD phase diagram by ? Locating critical end point (Lacey) See You ZHOU’s talk

28. Go metastable (T. Cohen) Outlook II: Invading the Bound

29. Invading the bound (T. Cohen) Outlook

30. Go Finite N O(1/N) effect, Higher derivative gravity, ( Brigante, Liu, Myers, Shenker, Yaida; Kats, Petrov )

31. Outlook III: Cold Atoms John Thomas’ Exps Damping in the trap T 0 /T F Free expanding w/ an initial angular velocity

32. Outlook III: Cold Atoms NR AdS/CFT Cold Unitary Atoms Adams, Balasubramanian, McGreevy; Maldacena, Martelli, Tachikawa; Herzog, Rangamani, Ross, 2008 d = 2 + 1 Not for cold unitary fermions at 2+1 d, where unitary fermi gas is a free gas JWC, Wen, 08

33. Outlook IV: PQGP still? Gluon viscosity: need gg gg, gg ggg Xu & Greiner: R23 ~ 7 R22 (PQGP) Arnold et al.: R23 ~0.1 R22 (SQGP)

34. Outlook IV: PQGP still? Gluon viscosity: need gg gg, gg ggg Xu & Greiner: R23 ~7 R22 (PQGP), parton cascade, soft bremss., massless external legs, LPM Arnold et al.: R23 ~ 0.1 R22 (SQGP), near collinear bremss., massive external legs, Boltzmann Eq. Chen, Dong, Ohnishi & Wang: soft bremss., massless external legs, LPM, Boltzmann eq., R23 ~(0.3-3.5) R22, sensitive to phase space

35. QCD Phase Diagram

36. The “Landscape” JWC, Li, Liu, Nakano; Itakura, Morimatsu, Otomo

37. The “Landscape” JWC, Li, Liu, Nakano