1. Heavy Flavor in Hot QCD Matter Ralf Rapp Cyclotron Institute + Dept. of Physics & Astronomy Texas A&M University College Station, TX USA Sapore Gravis Workshop 2014 Padova (Italy), 09.-12.12.14

2. 1.) Introduction: A “Calibrated” QCD Force  Vacuum charm-/bottomonium spectroscopy well described Confinement ↔ linear part of potential nonperturbative treatment: potential approach in medium (?) connect quarkonia and heavy-flavor diffusion in QGP [Kaczmarek et al ‘03] V [½ GeV] r [½ fm]

3. 1.) Introduction 2.) Heavy-Quark Interactions in QGP 3.) Open Heavy-Flavor Transport 4.) Quarkonium in p-A 5.) Conclusions Outline

4. 2.1 Free vs. Internal Energy in Lattice QCD strong QQ potential, U = ‹H int › large m Q * ~ m Q + U 1 (∞,T)/2 [Kaczmarek +Zantow ’05] - - F 1 (r,T) = U 1 (r,T) – T S 1 (r,T) weak QQ potential small m Q * ~ m Q + F 1 (∞,T)/2 F, U, S thermodynamic quantities Entropy: many-body effects Free Energy Internal Energy

5. 2.2 Reconstructed Potential from Lattice QCD real part ~ singlet free energy imaginary part ~ HTL perturbative  weakly coupled QGP?! Real Part Imaginary Part [Burnier et al ’14] static potential from Wilson loop correlator:

6. Lippmann-Schwinger equation In-Medium Q-Q T-Matrix: - 2.3 Thermodynamic Heavy-Quark T-Matrix in QGP thermal 2-particle propagator: single-quark selfenergy: simultaneous treatment of: - bound + scattering states - quarkonia (QQ) + open heavy flavor (Qq,Qg) QQ q,g = [Cabrera+RR ’06, Riek+RR ‘10]

7. 2.3.2 Free Energy in Potential Approach Key ingredients: imaginary parts + their  dependence adopt heavy-quark selfenergies from previous T-matrix calculations [S.Liu+RR in progress ] Euclidean T-matrix in static limit Spectral Function Free Energy [S.Liu+RR in prep]

8. 2.3.3. Free + Internal Energy from T-Matrix long-range confining force smaller in-medium quark mass relative to internal energy 1.2 T c 1.5 T c 2 T c U F V lat. F r [fm] potential ansatz:

9. 2.3.4 Brueckner Theory of Heavy Flavor in QGP 2-body potential QQ T-matrix Qq T-matrix Q → Q 0-modes Quark selfenergy QQ evolution (rate equation) Q spectra + v 2 (Langevin) spectral fcts./ eucl. correlat. quark-no. susceptibility lattice data exp. data Input Process Output Test - - lattice-QCD free energy

10. 1.) Introduction 2.) Heavy-Quark Interactions in QGP 3.) Open Heavy-Flavor Transport 4.) Quarkonium in p-A 5.) Conclusions Outline

11. 3.1 Heavy-Light Scattering Amplitudes confining force induces “Feshbach resonance” in Qq T-matrix strength comparable to previous internal-energy (U) potential c-q - New Potential V U-Potential

12. 3.2 Charm-Quark Relaxation Rates heavy-light T-matrix → HQ transport  c  [1/fm] HQ transport with V comparable to U inverted temperature dependence;  c ≈ 3 fm/c close to T c 3-momentum dependence: transition strong → weak [Riek+RR ’10, Huggins+RR ‘12] New Potential V U-Potential [Liu+RR in prep] p [GeV]

13. 3.3 D-Meson Transport in Hadronic Matter consistent with: - unitarized HQET (pion gas) - recent works in HRG using similar methods effective D-h scattering amplitudes [He,Fries+RR ’11]  D  [fm -1 ] [Cabrera et al ‘11] hadron gas at ~T c :  D ≈ 10fm/c  D  [fm -1 ] [Tolos+Torres-Ricon ’13, Ovzechuk et al‘14]

14. 3.4 Summary of Charm Diffusion in Matter shallow minimum near T c !? Quark-Hadron continuity!?  Hadronic Matter vs. QGP vs. Lattice QCD [He et al ’11, Riek+RR ’10, Ding et al ‘11, Gavai et al ‘11] AdS/QCD [Gubser ‘07] D s =T/m 

15. | | 3.5 Heavy-Quark Evolution in URHICs no “discontinuities” in interaction  diffusion toward T pc and hadronization same interaction (confining!) initial cond. (shadowing, Cronin), pre-equil. fields c-quark diffusion in QGP liquid c-quark hadronization D-meson diffusion in hadron liquid  c D  [fm/c] 0 0.5 5 10

16. 3.6.1 Heavy-Flavor Electrons at √s=62GeV importance of flow + Cronin effect at lower energies

17. 3.6.2 Heavy-Flavor Electrons at √s=62GeV uncertainties in pp baseline predict large medium effects in R AA and v 2

18. 4.) Charmonium:  ’(3686) easy to dissociate even in hadronic matter: , ,... +  ’ →DD,  ’ → D med D med [Grandchamp +RR ‘02 ] hadronic  ’ dissociation at SPS important ingredient for transport models [Sorge et al ‘97, …] [PBM+Stachel ‘00]

19. 4.2 Charmonium in d-Au “standard” procedure for fireball rate equation →  ’ suppression from hot medium similar in spirit to comover approach formation time effects?! [X.Du+RR,in prep ] [Ferreiro ‘14 ] [Liu et al ‘14 ]

20. 5.) Conclusions New insights into heavy-quark potential in QGP Importance of (large) imaginary parts Remnants of confinement essential for strong coupling “Critical” consequences for heavy-flavor diffusion (quarkonia tbd) Continuity + minimum of transport coefficient through T pc No principal difference between diffusion forces + hadronization Final-state interactions for quarkonia in p-A?

21. 3.) Quarkonium Transport in Heavy-Ion Collisions J/  D D - c - c [PBM+Stachel ’00,Thews et al ’01, Grandchamp+RR ‘01, Gorenstein et al ’02, Ko et al ’02, Andronic et al ‘03, Zhuang et al ’05, Ferreiro et al ‘11, …] J/  + g c + c + X ← → - Inelastic Reactions: detailed balance: Theoretical Input: Transport coefficients - chemical relaxation rate   - equililbrium limit N  eq (   B, m c *,  c eq ) Phenomenological Input: - J/ ,  c,  ’+c,b initial distributions [pp, pA] - space-time medium evolution [AA: hydro,...] Rate Equation: Observables

22.  c from fixed cc number: interplay of m c * and constrain spectral shape by lattice-QCD correlators 3.1 Thermal Charmonium Properties mc*mc* BB (a) Equilibrium  number: -  q (b) Inelastic  Width controlled by  s (parameter)

23. 3.2 Incomplete c-Quark Thermalization regeneration sensitive to charm-quark spectra [Song,Han, Ko ‘12 ] [Zhao+RR ‘11] Relaxation time ansatz: N  eq (  ) ~ N  therm (  ) · [1-exp(-  /  c eq )] Microscopic Calculation Impact on Regeneration

24. 3.3 Inclusive J/  at SPS + RHIC Fix two main parameters:  s ~0.3, charm relax.  c eq = 4(2) fm/c for U(F) vs. ~5(10) from T-matrix Strong Binding (U) Weak Binding (F) [Zhao+RR ‘10]

25. 3.4 J/  Excitation Function: BES at RHIC [Grandchamp +RR ’02 ] suppression pattern varies little (expected from transport) quantitative pp + pA baseline critical to extract systematics PHENIX (forward y) STAR (central y)

26. 3.5 J/  Predictions at LHC regeneration becomes dominant uncertainties in  cc +shadowing [Zhao+RR ‘11 ] low p T maximum confirms regeneration too much high-p T suppression?

27. 3.6  (1S) and  (2S) at LHC sensitive to color-screening + early evolution times clear preference for strong binding (U potential) similar results by possible problem in rapidity dependence  (1S) →  (2S) → [Grandchamp et al ’06, Emerick et al ‘11] Weak Binding Strong Binding [Strickland ‘12 ]

28. 3.7 Summary of Phenomenology Quarkonium discoveries in URHICs: - increase of J/  R AA SPS, RHIC → LHC - low-p T enhancement - sizable v 2 - increasing suppression of  ’ (  B  ’ ~  B J/  ) Implications - T 0 SPS (~230) < T diss (J/ ,  ’) < T 0 RHIC (~350) < T 0 LHC (~550) ≤ T diss (  ) - confining force screened at RHIC+LHC - marked recombination of diffusing charm quarks at LHC Fair predictive power of theoretical modeling - based on description of SPS+RHIC with 2 main parameters

29. 3.2.2 J/  at LHC: v 2 further increase at mid-y [He et al ’12 ]

30. 3.1.2 J/  p T Spectra + Elliptic Flow at RHIC small v 2 limits regeneration, but does not exclude it (strong binding) shallow minimum at low p T high p T : formation time, b feeddown, Cronin

31. 3.2.2 D-Meson Thermalization at LHC to be determined…

32. 3.3.3 J/  at LHC III: High-p t – ATLAS+CMS underestimate for peripheral (spherical fireball reduces surface effects …) [Zhao+RR ‘11 ]

33. 3.3.4 Time Evolution of J/  at LHC finite “cooking-time” window, determined by inelastic width [Zhao+RR ‘11 ] Strong Binding (U) Weak Binding (F)

34. 3.3 Charm-Quark Susceptibility in QGP sensitive to in-medium charm-quark mass finite-width effects can compensate in-medium mass increase [Riek+RR ‘10] 2 → →  → 0 m « T

35. 4.3 J/  at Forward Rapidity at RHIC [Zhao+ RR ‘10]

36. 4.2.Thermalization Rate from T-Matrix thermalization 4 (2) times faster using U (F) as potential than pert. QCD momentum dependence essential (nonpert. effect ≠ K-factor!) [Riek+RR ‘10]  c [1/fm]