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AdSCFT and transport constants in Expanding QGP

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... gravity duality. D-brane AdS ... in the frame following a particle. Boundary. Horizon. Equation of Motion ... Normalization of wave function. Result ... – PowerPoint PPT presentation

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Title: AdSCFT and transport constants in Expanding QGP


1
AdS/CFT and transport constants in Expanding
QGP
  • SangJin Sin (Hanyang)
  • _at_YITP, 2008.2.11

0707.0601 KY.Kim, SJS, I.Zahed Casalderry-solana
, Teaney,(ph/0605199) Janik,Peschansky,(th/060614
9)
2
SQGP in RHIC
  • RHIC found Unexpected strong nature of
    interaction in high energy collision.
  • Only Lattice or other non-perturbative method can
    do something for it.
  • String duality is one of such method.

3
Idea of calculation
  • Set up Langevin to introduce transport
    coefficients.
  • Identify noise correlation functionas two point
    function ltFFgt.
  • Use ads/cft to calculate ltFFgt

4
Langevin eq.
5
Noise v.s Force
6
Open/closed duality
  • Open string ? gauge theory
  • Closed string? gravity
  • Cylinder diagram
  • ?quantum gauge/classical gravity duality

7
D-brane AdS/CFT
  • D-brane closed string soliton whose vibration is
    restricted as open string vibration.
  • Multiple D-branes
  • Open st.?U(N)
  • Closed st.?extra-dim.?Holographicwarped
    transverse space? AdS

8
Holographic relation
YM?4d Boundary(global co-ord.)
5d AdS bulk
9
Finite temperature YM AdS Black hole
Expanding boundary Medium ??Falling
horizon (conformal invariance)
10
RHIC and Bjorken set up
Relativistically accelerated heavy nuclei
Central Rapidity Region
  • one-dimensional expansion.

11
Bjorken System
  • Longitudinal Position ??velocity.
  • All particles has common proper time
  • ? as coordinate

12
Bjorken frame
  • a frame following the particle
  • Bjorken frame is comoving frame.
  • Milnor Universe

13
Relativistic Hydrodynamics
  • Bjorken framelocal rest frame
  • where u(1,0,0,0)
  • simplies !
  • Hydro eq.
  • ?

14
Gravity dual of Bjorken system
  • Find a solution of Einstein eq. in AdSwith zero
    5d energy-momentum tensor.with falling horizon
    as BC.
  • Use Hologrphic renormalization to find the
    relation of 5d metric and boundary energy
    momentum tensor.
  • Such sol. found by JanikPeschanskySuch sol.
    with viscousity found by
    SJS Nakamura

15
Janik-Peschansky sol.
? Falling Horizon solution as desired!
16
Quasi-static Form of metric
17
New time
18
String fluctuation in the frame following a
particle
Boundary
Horizon
19
Equation of Motion
20
Reduced Boundary action
21
Eq.of M for
22
Retarded Green FunctionAnd Boundary condition
Need Infalling boundary condition for
23
Scheme of Calculation
24
The key problem
Infalling fcts are Needed here
u0
Infalling fcts are easily found here
horizon
25
Stratege of work
26
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27

28
Normalization of wave function
29
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30
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31
Result
32
Decorrelation time
33
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34
Momentum correlation and Diffusion constant
35
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36
Diffusion Rate
37
Solution
Cross over is Exponential
38
Conclusion
  • We considerred Diffusion of heavy quark in a
    expanding medium
  • In comoving frame time dependent diffusion
    problem is captured in the retarded Green
    function, which is calculated by AdS/CFT
  • Equilibrium is reached exponentially fast.With
    time scale

39
Hankel transform
40
Hydrodynamic Limit
41
WKB Limit
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