1 / 61

Jet correlations at RHIC via AdS/CFT

Jet correlations at RHIC via AdS/CFT. (and entropy production). Amos Yarom, Munich. together with: S. Gubser and S. Pufu. TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: A A A A A A A A A A A. The quark gluon plasma at RHIC. Measuring jets. .

carrington
Download Presentation

Jet correlations at RHIC via AdS/CFT

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Jet correlations at RHIC via AdS/CFT (and entropy production) Amos Yarom, Munich together with: S. Gubser and S. Pufu TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAAAAAAAAAA

  2. The quark gluon plasma at RHIC

  3. Measuring jets

  4.  Measuring jets

  5. =p Measuring di-jets

  6. (STAR, 0701069) Measuring di-jets

  7. (STAR, 0701069) Measuring di-jets =

  8. (STAR, 0701069) Measuring di-jets »-1

  9. Creation of sound waves (Casalderrey-Solana, Shuryak, Teaney, 2004, 2006)

  10. Creation of sound waves (Casalderrey-Solana, Shuryak, Teaney, 2004, 2006)

  11. Mach cones and di-jets (Casalderrey-Solana, Shuryak, Teaney, 2004, 2006) »-1

  12. AdS5 CFT AdS/CFT J. Maldacena N=4 SYM plasma via AdS/CFT Vacuum Empty AdS5 gYM2 N L4/’2 L3/2 G5 N2 J. Maldacena hep-th/9711200

  13. AdS5 CFT T>0 N=4 SYM plasma via AdS/CFT Empty AdS5 Thermal state Vacuum AdS5 BH gYM2 N L4/’2 L3/2 G5 N2 Horizon radius Temperature J. Maldacena hep-th/9711200 E. Witten hep-th/9802150

  14. 0 x1 xi, t AdS5 CFT Thermal state AdS5 BH gYM2 N L4/’2 z0 1/ T z0 L3/2 G5 N2 z Horizon radius Temperature E. Witten hep-th/9802150 AdS Black holes

  15. AdS5 CFT z0 AdS/CFT J. Maldacena Static quarks (Maldacena, 1996) 0 ? ? Heavy quark Endpoints of an open string J. Maldacena hep-th/9803002 z

  16. AdS5 CFT z0 Moving quarks (Holzhey, Karch, Kovtun, Kozcaz, Yaffe, 2006, Gubser 2006, Teaney Cassalderrey-Solana, 2006) 0 ? Massive parton Endpoints of an open string J. Maldacena hep-th/9803002 z

  17. AdS5 CFT z0 The energy momentum tensor 0 Gubser, Klebanov, Polyakov hep-th/9802109 Witten hep-th/9802150 De Haro, Solodukhin, Skenderis, hep-th/0002230 z

  18. 0 AdS5 CFT z0 z Metric fluctuations AdS black hole The energy momentum tensor Gmn(z,k) Gubser, Klebanov, Polyakov hep-th/9802109 Witten hep-th/9802150 De Haro, Solodukhin, Skenderis, hep-th/0002230

  19. z0 The energy momentum tensor (Friess, Gubser, Michalogiorgakis, Pufu, 2006) 0 z

  20. Energy density for v=3/4 (Gubser, Pufu, AY, 2007 Chesler, Yaffe, 2007) Over energy Under energy

  21. v=0.75 v=0.58 v=0.25

  22. Small momentum approximations (Friess, Gubser, Michalogiorgakis, Pufu, 2006 Gubser, Pufu, AY, 2007)

  23. k(iSj) =1/2(ki Sj+kj Si)-1/3 ij kl Sl = <T00> s = 4 /3  Sj = -<T0j> The hydrodynamic approximation (Casalderrey-Solana, Shuryak, Teaney, 2004, 2006) Large distances – linear hydrodynamic picture valid Intermediate distances – nonlinear hydrodynamics Short distances – Strong dissipative effects

  24. Energy density for v=3/4

  25. 0

  26. Short distance asymptotics (Gubser, Pufu, 2007, AY, 2007)

  27. Wakes

  28. Mach cones, wakes and di-jets (Casalderrey-Solana, Shuryak, Teaney, 2004, 2006)

  29. (STAR, 0701069) Mach cones, wakes and di-jets (Casalderrey-Solana, Shuryak, Teaney, 2004, 2006)

  30. (STAR, 0701069) Mach cones, wakes and di-jets (Casalderrey-Solana, Shuryak, Teaney, 2004, 2006) Jhydro=(e0, g0, 0, 0) Jhydro=(0, k1, k2, k3)g1

  31. 0 z0 z The Poynting vector

  32. The Poynting vector (Gubser, Pufu, AY, 2007 Chesler, Yaffe, 2007) S? S1 V=0.25 V=0.58 V=0.75

  33. Sound Waves Small momentum asymptotics (Friess, Gubser, Michalogiorgakis, Pufu, 2006 Gubser, Pufu, AY, 2007) Wake

  34. Comparison with the phenomenological model (Casalderrey-Solana, Shuryak, Teaney, 2004, 2006) V=0.75

  35. Energy analysis (Friess, Gubser, Michalogiorgakis, Pufu, 2006 Gubser, Pufu, AY, 2007)

  36. z0 F Just been calculated 0 z Energy analysis (Friess, Gubser, Michalogiorgakis, Pufu, 2006 Gubser, Pufu, AY, 2007) ?

  37. Energy analysis

  38. Energy analysis =

  39. (STAR, 0701069) = Energy analysis 25-30

  40. z0 Other theories (Gubser, AY,2007) 0 z

  41. z0 Other theories (Gubser, AY, 2007) (Yaffe, Chesler, 2007) 0 z

  42. (STAR, nucl-ex/0701069) Mach cones, wakes and di-jets (STAR, 0510055) (PHENIX, 0611019) 0.15 GeV<p?<4 GeV

  43. Mesons (Gubser, Pufu, AY,2007) 0 z0 z

  44. l l → → v v Mesons (Gubser, Pufu, AY,2007) 0 z0 z

  45. Mesons (Gubser, Pufu, AY,2007) 0 z0 z

  46. 0 0 z0 z0 z Mesons (Gubser, Pufu, AY,2007)

  47. u d s c t b Mesons (?) (Gubser, Pufu, AY,2007) ? ? M > T

  48. 0 z0 z General analysis (Gubser, AY,2008) J Dh=J 1) J» O(z-1) 2) rJ=0 3) “Causal” Dh=J 10

  49. 0 z0 z General analysis (Gubser, AY,2008) Dh=J Fine print Fine print

  50. 0 z0 z General analysis (Gubser, AY,2008) Dh=J

More Related