Heavy Quark Diffusion with Relativistic Langevin Dynamics in the Quark-Gluon Fluid
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Transcript of Heavy Quark Diffusion with Relativistic Langevin Dynamics in the Quark-Gluon Fluid
Heavy Quark Diffusion with Relativistic Langevin Dynamics in the Quark-
Gluon Fluid
Yukinao Akamatsu 赤松 幸尚(Univ. of Tokyo)
ATHIC 2008 Tsukuba
Ref : YA, T. Hatsuda, and T. Hirano, arXiv:0809.1499[hep-ph]
Outline
• Introduction• Langevin Dynamics of Heavy Quarks• Hydro + HQ Model• Numerical Results• Conclusions and Outlook
relativistic ideal hydrodynamics
Light (m << T~200MeV) components (g, u, d, s)
• Relativistic Heavy Ion Collision
1. Introduction
Heavy (M >> T~200MeV) components (c, b)long time scale not thermalized in fluid impurity
HQ
g,u,d,s
Other impurities : J/Ψ (color singlet), Jet (too energetic)
strongly coupled matter
2. Langevin Dynamics of Heavy Quarks
• Heavy Quarks in Medium
1. weak coupling (pQCD)
2. strong coupling (AdS/CFT)
drag force
Energy loss of heavy quarks
energy of HQ dominant mechanism
low energy collision
high energy radiation
<Energy loss of HQ>
HQ q-hats > LQ q-hats indicates collision
but poor convergence
(Armesto ’06, Wicks ‘07)
(Caron-Huot ‘08)
(Gubser ’06,’07, HKKKY ’06, Teaney ‘06)
,
relativistic Langevin equation
Model of HQ in medium
the only input,dimensionless
in the rest frame of matter
22 6.7 2.2
72 21 7.2
assume isotropic noise
relaxation time of HQ
(at T=210MeV)
3. Hydro + HQ Model
• Flowchart
0 fm….
0.6 fm…
Little Bang
Initial Condition
Brownian Motion
Heavy Quark Spectra
Full 3D hydrodynamics
Electron Spectra
T(x), u(x)
Local temperature and flow
(pp + Glauber)
(Hirano ’06)
c(b)→D(B)→e- +νe+π etc_
time
QG
P
Experiment
(PHENIX, STAR ’07)
• Comments
Initial condition
available only spectral shape above pT~3GeV
<HQ in pp>
<decayed electron in pp>
No nuclear matter effects in initial conditionNo quark coalescence effects in hadronizationWhere to stop in coexisting phase at 1st order P.T. 3 choices (no/half/full coexisting phase)
Reliable at high pT
4. Numerical Results
• Profile of HQ Diffusion
2 time scales
22 6.7 2.2
72 21 7.2
Charm ~ not yet fully thermalizedBottom ~ not thermalized at all
: stay time and relaxation time
<relaxation times>
<stay times>
stay time :~3-4fm
• HQ Spectra
Nuclear modification factor
Large pT, γ large momentum loss large suppression
Elliptic flow
High pT (almost) no anisotropyAt low pT, large γ large anisotropy
• Electron Spectra
Bottom ratio
At pT above 3GeV, bottom origin electrons dominate.
Nuclear modification factor
Elliptic flow
Poor statistics for both simulation and experiment at high pT.But at least consistent.(Still preliminary, PHENIX : v2~0.05-0.1 for pT~3-5GeV)
Quite Large v2
5. Conclusions and Outlook
• Heavy quark can be described by relativistic Langevin dynamics with a parameter predicted by AdS/CFT.
• Prediction for heavy quark correlations.
• Latest experimental data for v2 seems to have larger elliptic flow.
• Theoretically, heavy quark energy loss at strong coupling (based more on field theory) should be reconsidered.
Back Up Slides
Average Temperature
charm bottom
Momentum Loss
charm bottom
RAA of Electrons from Charm/Bottom
charm bottom