Qualitative and Quantitative Energy Loss?

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Presentation transcript:

Qualitative and Quantitative Energy Loss? W. A. Horowitz University of Cape Town December 9, 2010 With many thanks to Brian Cole, Miklos Gyulassy, Ulrich Heinz, Jangyong Jia, and Yuri Kovchegov 11/29/2018 Kruger2010

Four Fundamental Forces Electromagnetism Gravity starchild.gsfc.nasa.gov John Maarschalk, travelblog.portfoliocollection.com Weak Strong lhs.lps.org/staff/sputnam/chem_notes/tritium_decay.gif 11/29/2018 Kruger2010

E&M Particle Physics Well Understood Lagrangian known: QED Vertex: Ex. of Precision QED: g - 2 Gabrielse et al., PRL97 (2006) Hanneke, Fogwell, and Gabrielse, PRL100 (2008) 11/29/2018 Kruger2010

E&M and Phase Diagrams Many body physics less well understood Water Hydrogen www.sv.vt.edu/classes/MSE2094_NoteBook/96ClassProj/examples/triplpt.html Calculated, Burkhard Militzer, Diploma Thesis, Berlin, 2000 11/29/2018 Kruger2010

QCD Particle Physics Well Understood Lagr. known: QCD Vertices: Qual. & Quant. agreement w/ data ALEPH, PLB284 (1992) PDG 11/29/2018 Kruger2010

What Are We Interested In? Measure many-body physics of strong force Test & understand theory of many-body non-Abelian fields Do this via Heavy Ion Collisions Unique as compared to strongly coupled Abelian problems Long Range Plan, 2008 11/29/2018 Kruger2010

Big Bang vs. Little Bang t = - ¥ t = 0 t = 1 fm/c t = 3 fm/c ALICE Collaboration t = - ¥ t = 0 t = 1 fm/c t = 3 fm/c t = 4 fm/c t = + ¥ JET Initial State Initial Overlap Thermalization QGP Hadronization Hadron Gas 11/29/2018 Kruger2010

QGP Energy Loss Learn about E-loss mechanism Most direct probe of DOF AdS/CFT Picture pQCD Picture 11/29/2018 Kruger2010

pQCD Rad Picture Bremsstrahlung Radiation Weakly-coupled plasma Medium organizes into Debye-screened centers T ~ 250 MeV, g ~ 2 m ~ gT ~ 0.5 GeV lmfp ~ 1/g2T ~ 1 fm RAu ~ 6 fm 1/m << lmfp << L mult. coh. em. Gyulassy, Levai, and Vitev, NPB571 (2000) LPM dpT/dt ~ -LT3 log(pT/Mq) Bethe-Heitler dpT/dt ~ -(T3/Mq2) pT 11/29/2018 Kruger2010

High-pT Observables Naively: if medium has no effect, then RAA = 1 Common variables used are transverse momentum, pT, and angle with respect to the reaction plane, f pT f , g, e- Fourier expand RAA: 11/29/2018 Kruger2010

Expectations from pQCD Power law p + p p + X spectrum ds/dpT ~ A/(pT)n pQCD fractional energy loss e ~ log(pT)/pT For n fixed, RAA 1 at large pT => RAA ~ (1 – e)n-1 pT n RHIC glue LHC glue RHIC light quarks LHC light quarks pT n At RHIC, n increases with pT; at LHC, n relatively constant 11/29/2018 Kruger2010

pQCD Success at RHIC: (circa 2005) Null Control: RAA(g)~1 Y. Akiba for the PHENIX collaboration, Nucl. Phys. A774 (2006) 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 11/29/2018 Kruger2010

pQCD Suppression Picture Inadequate Lack of even qualitative understanding p0, h, g RAA well described, BUT e- RAA, v2 are not, even with elastic loss PHENIX, Phys. Rev. Lett. 98, 172301 (2007) Wicks, WAH, Djordjevic, Gyulassy, NPA784, 2007 11/29/2018 Kruger2010

Death of pQCD at RHIC? Failure at > 9 GeV! Pert. at LHC energies? Important to get to >~ 10 GeV to avoid IS, hadronization effects Rui Wei, for PHENIX, QM09 PHENIX, arXiv:1006.3740 Pert. at LHC energies? 11/29/2018 Kruger2010

Before We Make Any Conclusions... While experiments are converging Theoretically, what are the effects of higher orders in as (large) kT/xE (large) MQ/E (large?) opacity (large?) geometry uncertainty in IC (small) coupling to flow (large?) better treatment of elastic E-loss E-loss in confined matter 11/29/2018 Kruger2010

ALICE First Results! Rise with pT looks very pQCD-ish 5.5 TeV WAH, Int.J.Mod.Phys. E16 (2007) 5.5 TeV ALICE, arXiv:1012.1004 11/29/2018 Kruger2010

Caution about pQCD at LHC Albacete and Marquet, PLB687, 2010 RpPb ~ 0.5! Quenching due to IS or FS? Initial or Final State physics? Require exp. control over production RPbPb ~ 0.25 from IS alone! p + p and p + Pb run at LHC 11/29/2018 Kruger2010

Jets in AdS/CFT Model heavy quark jet energy loss by embedding string in AdS space dpT/dt = - m pT m = pl1/2 T2/2Mq J Friess, S Gubser, G Michalogiorgakis, S Pufu, Phys Rev D75 (2007) Similar to Bethe-Heitler dpT/dt ~ -(T3/Mq2) pT Very different from usual pQCD and LPM dpT/dt ~ -LT3 log(pT/Mq) 11/29/2018 Kruger2010

Compared to Data String drag: qualitative agreement WAH, PhD Thesis 11/29/2018 Kruger2010

Light Quark and Gluon E-Loss WAH, in preparation Marquet and Renk, PLB685 (2010) SS Gubser, QM08 DLgtherm ~ E1/3 DLqtherm ~ (2E)1/3 Gubser et al., JHEP0810 (2008) Chesler et al., PRD79 (2009) 11/29/2018 Kruger2010

pQCD vs. AdS/CFT at LHC Plethora of Predictions: WAH, M. Gyulassy, PLB666 (2008) Taking the ratio cancels most normalization differences pQCD ratio asymptotically approaches 1, and more slowly so for increased quenching (until quenching saturates) AdS/CFT ratio is flat and many times smaller than pQCD at only moderate pT WAH, M. Gyulassy, PLB666 (2008) 11/29/2018 Kruger2010

Worldsheet boundary Spacelike if g > gcrit Not So Fast! Speed limit estimate for applicability of AdS drag g < gcrit = (1 + 2Mq/l1/2 T)2 ~ 4Mq2/(l T2) Limited by Mcharm ~ 1.2 GeV Similar to BH LPM gcrit ~ Mq/(lT) No Single T for QGP smallest gcrit for largest T T = T(t0, x=y=0): “(” largest gcrit for smallest T T = Tc: “]” D3 Black Brane D7 Probe Brane Q Worldsheet boundary Spacelike if g > gcrit Trailing String “Brachistochrone” “z” x5 11/29/2018 Kruger2010

LHC RcAA(pT)/RbAA(pT) Prediction (with speed limits) WAH, M. Gyulassy, PLB666 (2008) T(t0): “(”, corrections likely small for smaller momenta Tc: “]”, corrections likely large for higher momenta Qualitatively, corrections to AdS/CFT result will drive double ratio to unity 11/29/2018 Kruger2010

Conclusions Energy loss is a unique tool for probing QGP pQCD fails to simultaneously describe RAA, v2, ... for p, e at RHIC Importance of HO effects, approx.,...? Exciting new ALICE results Appears tantalizingly perturbative Due to final state energy loss or initial state? 2.76 TeV p + p and p + Pb run required for interp. Heavy Quarks provide clean observable for investigating QGP physics 11/29/2018 Kruger2010