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William Horowitz Columbia University

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Presentation on theme: "William Horowitz Columbia University"— Presentation transcript:

1 Possible String Theoretic Deviations from pQCD in Heavy Quark Energy Loss at LHC
William Horowitz Columbia University Frankfurt Institute for Advanced Studies (FIAS) May 21, 2007 With many thanks to Miklos Gyulassy. CERN Heavy Ion Forum

2 pQCD Success at RHIC: (circa 2005) Consistency: RAA(h)~RAA(p)
Y. Akiba for the PHENIX collaboration, hep-ex/ Consistency: RAA(h)~RAA(p) Null Control: RAA(g)~1 GLV Prediction: Theory~Data for reasonable fixed L~5 fm and dNg/dy~dNp/dy CERN Heavy Ion Forum

3 Trouble for wQGP Picture
D. Teaney, Phys. Rev. C68, (2003) Hydro h/s too small v2 too large A. Drees, H. Feng, and J. Jia, Phys. Rev. C71: (2005) (first by E. Shuryak, Phys. Rev. C66: (2002)) e- RAA too small M. Djorjevic, M. Gyulassy, R. Vogt, S. Wicks, Phys. Lett. B632:81-86 (2006) CERN Heavy Ion Forum

4 Strong Coupling The supergravity double conjecture: QCD  SYM  IIB
IF super Yang-Mills (SYM) is not too different from QCD, & IF Maldacena conjecture is true Then a tool exists to calculate strongly-coupled QCD in SUGRA CERN Heavy Ion Forum

5 Qualitative AdS/CFT Successes:
sstrong=(3/4) sweak, similar to Lattice h/sAdS/CFT ~ 1/4p << 1 ~ h/spQCD e- RAA ~ p, h RAA; e- RAA(f) Mach wave-like structures Give up on pQCD? CERN Heavy Ion Forum

6 Ideal Hydro? pQCD elastic: h/s ~ 1
Hydro merely propagates initial conditions; its results are highly dependent on them pQCD elastic: h/s ~ 1 pQCD r+e PC: h/s ~ .1? AdS: universal lower bound for all infinitely coupled systems h/s ~ 1/4p Glauber initial state => ideal (ST) hydro CGC initial state => viscous (pQCD) hydro T. Hirano, U. W. Heinz, D. Kharzeev, R. Lacy, Y. Nara, Phys. Lett. B636: (2006) Must understand initial state better before reaching a conclusion: A. Adil, M. Gyulassy, T. Hirano, Phys. Rev. D73: (2006) CERN Heavy Ion Forum

7 Simultaneous p, e- Suppression
pQCD is not falsified: Elastic loss? Uncertainty in c, b contributions In-medium fragmentation? Resonances? A. Adil and I. Vitev, hep-ph/ Naïve pQCD => large mass, small loss But p, h RAA ~ e- RAA! S. Wicks, WH, M. Gyulassy, and M. Djordjevic, nucl-th/ H. Van Hees, V. Greco, and R. Rapp, Phys. Rev. C73, (2006) CERN Heavy Ion Forum

8 Simultaneous RAA, v2 Description
Energy loss translates spatial anisotropy of medium to jets RAA and v2 are thus anti-correlated First seen for pions, no nonperturbative model reproduces both RAA and v2 Observed for e-, too No known solution to the puzzle PHENIX, Phys. Rev. Lett. 98, (2007) WH, Acta Phys. Hung. A27: GREL 40-50% MPC 30% CERN Heavy Ion Forum

9 AdS/CFT vs. pQCD with Jets
Langevin model Collisional energy loss for heavy quarks Restricted to low pT pQCD vs. AdS/CFT computation of D, the diffusion coefficient ASW model Radiative energy loss model for all parton species pQCD vs. AdS/CFT computation of Debate over its predicted magnitude ST drag calculation Equation for infinitely massive quark moving with constant v through infinitely coupled SYM at uniform T not yet used to calculate observables: let’s do it! CERN Heavy Ion Forum

10 Drag Picture The Heavy Quark Brachistochrone: CERN Heavy Ion Forum
J Friess, S Gubser, G Michalogiorgakis, S Pufu, Phys Rev D75:106003, 2007 CERN Heavy Ion Forum

11 Looking for a Robust, Detectable Signal
Use large LHC pT reach and identification of c and b to distinguish RAA ~ (1-e(pT))n(pT), where pf = (1-e)pi (i.e. e = 1-pf/pi) Asymptotic pQCD momentum loss: String theory drag momentum loss: Independent of pT and strongly dependent on Mq! T2 dependence in exponent makes for a very sensitive probe Expect: epQCD vs. eAdS indep of pT!! dRAA(pT)/dpT > 0 => pQCD; dRAA(pT)/dpT < 0 => ST erad ~ as L2 log(pT/Mq)/pT eST ~ 1 - Exp(-m L), m = pl1/2 T2/2Mq S. Gubser, Phys.Rev.D74: (2006) CERN Heavy Ion Forum

12 A Note on LHC pT Reach More on pT limits from the AdS side later
ALICE Physics Performance Report, Vol. II CERN Heavy Ion Forum

13 Regimes of Applicability
String Regime Large Nc, constant ‘t Hooft coupling ( ) Small quantum corrections Large ‘t Hooft coupling Small string vibration corrections Only tractable case is both limits at once Classical supergravity (SUGRA) RHIC/LHC Regime Mapping QCD Nc to SYM is easy, but coupling is hard aS runs whereas aSYM does not: aSYM is something of an unknown constant Taking aSYM = aS = .3 (D/2pT ~ 1); D/2pT ~ 3 => aSYM ~ .05 CERN Heavy Ion Forum

14 Models AdS/CFT Drag “Obvious”: as = aSYM, TSYM = TQCD D/2pT = 3 inspired: as = .05 pQCD/Hydro inspired: as = .3 (D/2pT ~ 1) “Alternative”: l = 5.5, TSYM = TQCD/31/4 WHDG convolved radiative and collisional energy loss as = .3 WHDG radiative energy loss (similar to ASW) = 40, 100 All use realistic, nonuniform medium with Bjorken expansion Two extrapolations to LHC: PHOBOS (dNg/dy = 1750); CGC (dNg/dy = 2900) CERN Heavy Ion Forum

15 LHC c, b RAA pT Dependence
LHC Prediction Zoo: What a Mess! Let’s go through step by step Naïve expectations born out in full numerical calculation: dRAA(pT)/dpT > 0 => pQCD; dRAA(pT)/dpT < 0 => ST Significant rise in RAA(pT) for pQCD Rad+El Large suppression leads to flattening Use of realistic geometry and Bjorken expansion allows saturation below .2 CERN Heavy Ion Forum

16 A Cleaner Signal But what about the interplay between mass and momentum? Take ratio of c to b RAA(pT) pQCD: Mass effects die out with increasing pT Ratio starts below 1, asymptotically approaches 1. Approach is slower for higher quenching ST: drag independent of pT, inversely proportional to mass Ratio starts below 1; independent of pT RcAA(pT)/RbAA(pT) ~ 1 - as n(pT) L2 log(Mb/Mc) ( /pT) CERN Heavy Ion Forum

17 LHC RcAA(pT)/RbAA(pT) Prediction
Recall the Prediction Zoo: Taking the ratio cancels most normalization differences seen previously pQCD ratio asymptotically approaches 1, and more slowly so for increased quenching (until quenching saturates) ST ratio is flat and many times smaller than pQCD at only moderate pT CERN Heavy Ion Forum

18 But There’s a Catch Speed limit estimate for applicability of AdS/CFT drag computation g < gcrit = (1 + 2Mq/l1/2 T)2 ~ 4Mq2/(l T2) Limited by Mcharm ~ 1.2 GeV Ambiguous T for QGP smallest gcrit for largest T = T(t0, x=y=0): (O) largest gcrit for smallest T = Tc: (|) CERN Heavy Ion Forum

19 LHC RcAA(pT)/RbAA(pT) Prediction (with speed limits)
O: corrections unlikely for smaller momenta |: corrections likely for higher momenta CERN Heavy Ion Forum

20 Zooming In Factor ~2-3 increase in ratio for pQCD
Possible distinction for Rad only vs. Rad+El at low-pT CERN Heavy Ion Forum

21 Additional Discerning Power
Adil-Vitev in-medium fragmentation rapidly approaches, and then broaches, 1 Does not include partonic energy loss, which will be nonnegligable as ratio goes to unity CERN Heavy Ion Forum

22 Conclusions PID and large pT reach will give the LHC a unique position to make discoveries in the heavy quark sector Year 1 of LHC could show qualitative differences between energy loss mechanisms: dRAA(pT)/dpT > 0 => pQCD; dRAA(pT)/dpT < 0 => ST Ratio of charm to bottom RAA will be an important observable Ratio is: flat in ST; asymptotically approaching 1 from below in pQCD While future AdS/CFT calculations could well alter the ST predictions shown here, it is highly unlikely that a pQCD mechanism can be found that allows mass effects to persist out to momenta orders of magnitude larger than Mq A measurement of this ratio NOT going to 1 will be a clear sign of new physics: pQCD predicts ~ 2-3 times increase in this ratio by 30 GeV—this can be observed in year 1 at the LHC CERN Heavy Ion Forum

23 Conclusions (cont’d) Additional LHC Goodies:
Adil Vitev in-medium fragmentation results in a much more rapid rise to 1 for RcAA/RbAA with the possibility of breaching 1 and asymptotically approaching 1 from above Surface emission models (although already unlikely as per v2(pT) data) predict flat in pT c, b RAA, with a ratio of 1 Mach cone may be due to radiated gluons: from pQCD the away-side dip should widen with increasing parton mass Moderately suppressed radiative only energy loss shows a dip in the ratio at low pT; convolved loss is monotonic. Caution: in this regime, approximations are violated CERN Heavy Ion Forum


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