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Understanding Energy Loss of Heavy Quarks

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Presentation on theme: "Understanding Energy Loss of Heavy Quarks"— Presentation transcript:

1 Understanding Energy Loss of Heavy Quarks
William Horowitz The Ohio State University June 2, 2009 With many thanks to Brian Cole, Yuri Kovchegov, and Ulrich Heinz 2009 RHIC and AGS Users’ Meeting

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Outline Introduction pQCD AdS/CFT pQCD Again Conclusions 2009 RHIC and AGS Users’ Meeting

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The Heavy Flavor Data STAR, Phys. Rev. Lett. 98, (2007) PHENIX, Phys. Rev. Lett. 98, (2007) 2009 RHIC and AGS Users’ Meeting

4 Simultaneous Understanding?
Y. Akiba for the PHENIX collaboration, hep-ex/ STAR, Phys. Rev. Lett. 98, (2007) WHDG C. Vale, QM09 Plenary (analysis by R. Wei) PHENIX, Phys. Rev. Lett. 98, (2007) 2009 RHIC and AGS Users’ Meeting

5 RAA vs. v2 Anti-correlation
WH, Acta Phys.Hung.A27: ,2006 p0 Cu+Cu PHENIX, arXiv: 2009 RHIC and AGS Users’ Meeting

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pQCD 2009 RHIC and AGS Users’ Meeting

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Hard Spectra PHENIX, [hep-ex] A Dion, Quark Matter 2009 pT [GeV/C] 1 9 J Dunlop, QM09 2009 RHIC and AGS Users’ Meeting

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pQCD Uncertainty (I) E-loss Mechanisms Initial Spectra S Wicks, et al., NPA784: ,2007 N Armesto, et al., Phys.Lett.B637: ,2006 S Wicks, Ph. D. Thesis 2009 RHIC and AGS Users’ Meeting

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pQCD Uncertainty (II) kT int. cutoff (UV) mg/IR kT cutoff B Cole and WH M Djordjevic, B Cole and WH, not-yet-published 2009 RHIC and AGS Users’ Meeting

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Initial State Effects Cronin for e-? Coal. + K P.B. Gossiaux, QM09; P.B. Gossiaux, R. Bierkandt, J. Aichelin, arXiv: 2009 RHIC and AGS Users’ Meeting

11 Out-of-Medium Hadronization Effects
Add’l Channels Coalescence R Rapp and H van Hees, arXiv: H. van Hees, M. Mannarelli, V. Greco, and R. Rapp, Phys.Rev.Lett.100:192301,2008 2009 RHIC and AGS Users’ Meeting

12 In-Medium Hadronization Effects
Coll. Diss. In-medium Frag. A Adil, I Vitev, Phys.Lett.B649: ,2007 A Adil and I Vitev, Phys.Lett.B649: ,2007 2009 RHIC and AGS Users’ Meeting

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AdS/CFT 2009 RHIC and AGS Users’ Meeting

14 Motivation for High-pT AdS
Why study AdS E-loss models? Many calculations vastly simpler Complicated in unusual ways Data difficult to reconcile with pQCD pQCD quasiparticle picture leads to dominant q ~ m ~ .5 GeV mom. transfers => Nonperturbatively large as Use data to learn about E-loss mechanism, plasma properties Domains of self-consistency crucial for understanding 2009 RHIC and AGS Users’ Meeting

15 AdS/CFT Energy Loss Models I
Langevin Diffusion Collisional energy loss for heavy quarks Restricted to low pT pQCD vs. AdS/CFT computation of D, the diffusion coefficient ASW/LRW model Radiative energy loss model for all parton species pQCD vs. AdS/CFT computation of Debate over its predicted magnitude Moore and Teaney, Phys.Rev.C71:064904,2005 Casalderrey-Solana and Teaney, Phys.Rev.D74:085012,2006; JHEP 0704:039,2007 BDMPS, Nucl.Phys.B484: ,1997 Armesto, Salgado, and Wiedemann, Phys. Rev. D69 (2004) Liu, Ragagopal, Wiedemann, PRL 97:182301,2006; JHEP 0703:066,2007 2009 RHIC and AGS Users’ Meeting

16 AdS/CFT Energy Loss Models II
String Drag calculations: Embed string rep. quark/gluon in AdS geom. Includes all E-loss modes (difficult to interpret) Gluons and light quarks Empty space HQ calculation Previous HQ: thermalized QGP plasma, temp. T HQ in Shock: hot and cold nuclear matter Gubser, Gulotta, Pufu, Rocha, JHEP 0810:052, 2008 Chesler, Jensen, Karch, Yaffe, arXiv: [hep-th] Kharzeev, arXiv: [hep-ph] Gubser, Phys.Rev.D74:126005,2006 Herzog, Karch, Kovtun, Kozcaz, Yaffe, JHEP 0607:013, 2006 WH and Y Kovchegov, arXiv: 2009 RHIC and AGS Users’ Meeting

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AdS Thermal Drag P Chesler, Quark Matter 2009 AdS/CFT Drag: dpT/dt ~ -(T2/Mq) pT WH, Ph. D. Thesis 2009 RHIC and AGS Users’ Meeting

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Shocking Loss HQ Drag in Hot and Cold nuclear matter Embedded String in Shock Q vshock x z Before After Recall for BH: Shock gives exactly the same drag as BH for L = p T 2009 RHIC and AGS Users’ Meeting

19 Future RHIC Measurements
In-Medium Frag WH, J.Phys.G35:044025,2008 2009 RHIC and AGS Users’ Meeting

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Hard to Beat PHENIX, Phys. Rev. Lett. 98, (2007) S S Gubser, Quark Matter 2009 2009 RHIC and AGS Users’ Meeting

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pQCD Again 2009 RHIC and AGS Users’ Meeting

22 pQCD as Consistent Picture?
v2 Sensitivity to IC A Drees, H Feng, J Jia, Phys.Rev.C71:034909,2005 2009 RHIC and AGS Users’ Meeting

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High e and pQCD h/s? T Hirano, et al., Phys.Lett.B636: ,2006 2009 RHIC and AGS Users’ Meeting

24 pQCD p and e- Consistency?
Coll. fluctuations Dyn. scat. centers M Djordjevic, QM09; M Djordjevic and U Heinz, PRL101:022302,2008 S Wicks, Ph. D. Thesis 2009 RHIC and AGS Users’ Meeting

25 Conclusions and Outlook
Exciting years ahead! Initial state effects Higher momenta Reduce hadronization effects Individual c and b contributions Disambiguate E-loss mechanisms HQ correlations Disambiguate E redistribution mechanisms Rehabilitation for pQCD? 2009 RHIC and AGS Users’ Meeting

26 2009 RHIC and AGS Users’ Meeting
Supplements 2009 RHIC and AGS Users’ Meeting

27 LHC RcAA(pT)/RbAA(pT) Prediction
Individual c and b RAA(pT) predictions: WH and M. Gyulassy, Phys. Lett. B 666, 320 (2008) WH and M. Gyulassy, Phys. Lett. B 666, 320 (2008) 2009 RHIC and AGS Users’ Meeting

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S Wicks, WH, M Djordjevic, and M Gyulassy, Nucl.Phys.A784: ,2007 2009 RHIC and AGS Users’ Meeting

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30 Energy Loss Comparison
D7 Probe Brane t z = 0 x v AdS/CFT Drag: dpT/dt ~ -(T2/Mq) pT Q, m zm = l1/2/2pm 3+1D Brane Boundary D3 Black Brane (horizon) zh = 1/pT Black Hole z = ¥ Similar to Bethe-Heitler dpT/dt ~ -(T3/Mq2) pT Very different from LPM dpT/dt ~ -LT3 log(pT/Mq) 2009 RHIC and AGS Users’ Meeting

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New Geometries Constant T Thermal Black Brane Shock Geometries Nucleus as Shock J Friess, et al., PRD75:106003, 2007 DIS Embedded String in Shock Before After Albacete, Kovchegov, Taliotis, JHEP 0807, 074 (2008) Q vshock x z vshock x z Q Bjorken-Expanding Medium 2009 RHIC and AGS Users’ Meeting

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