heavy quarkonium states with the holographic potential defu hou (ccnu) from strings to things,...
TRANSCRIPT
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Heavy Quarkonium States with the Holographic Potential
Defu Hou (CCNU)
From Strings to Things , Seattle , May 2008
With Hai-cang Ren, JHEP 0801:029,2008. 0710.2639
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OUTLINES
Introduction Holographic potential model from AdS/CFT Holographic potential model with IR cut.
Concluding remarks
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Many interesting phenomena in QCD lie in the strongly-coupled region.
Non-perturbative methods for analysis
Lattice: problematic with finite chemical potentioal, time-
dependent problems
AdS/CFT: Notable success in RHIC physics
Viscosity, Jet quenching, …
Introduction
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QCD Diagramm
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Heavy meson melting
• At T<Tc, confined ,potenial linearing rises• At T>Tc, deconf. Short range attraction
range: screening length Lsc
As T , ↗ Lsc , ↘ there exists a Td : the potential no
longer binding for T>Td ( Melting Temperature)
Heavy quakonium melting is an important signal of QGP
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Nonperturbative calculation of Td
• Potential model
Lattice F. Karsch , Brambilla…
AdS/CFT Maldacena, Rey, Liu , Avramis
• Spectral function
Lattice Karch
AdS/CFT Hoyos, Kim et al
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Holographic potential model from AdS/CFT
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Q Qr
1/Tt
Extracting V(r) from Wilson loop
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• F(r,t) is the free energy excess of a static pair of qq
The internal energy reads
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• F-ansatz
V(r) =F(r,T)
• U –ansatz
V(r)=U(r, T)
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Poential From Lattice • Quarkonium probes non-perturbative information about medium. How?
W (C) 1
NTr P exp i A
C
W (C)Texp iLtime E(L) E ren
• Wilson loop is static time-like and in fundamental representation:
• Wilson loop is calculable in lattice QCD
Bielefeld Group, hep-lat/0509001time
distance
L
Ltime
Matsui, Satz 1986
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Field Theory Gravity Theory=
Gauge TheoriesQCD
Quantum GravityString theory
the large N limitSupersymmetric Yang Mills
Gravitational theory in 10 dimensions
N large
Calculations Correlation functionsQuark-antiquark potential
Holography
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Potential from AdS/CFT
• According to the holographic principle, the thermal average of a Wilson loop operator in 4D N=4 SUSY YM at large N_c and large 't Hooft coupling corresponds to the minimum area of the string world sheet in the 5D AdS metric with a Euclidean signature,
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bounded by the loop C, when y goes to infinity, y->1 BH
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Minimizing the world sheet area (the Nambu-Goto action)
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qq r qq r
BH
+_
y
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Free energy
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Result of pentential
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Bound state & Schrődinger equation
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Numerical Results
• Value of ‘t Hooft coupling.
• Upper limit : QCD value of coupling at RHIC
• Lower limit: heavy quark potential , (Gubser)
• Mc=1.65Gev, Mb=4.85Gev, Tc=186MeV
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Dissociate Temperature
Td in MeV
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Holographic potential model with an IR cutoff
Hard Wall : Erlich, Katz, Son, Stephanov
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• In the hadronic phase
• In the plasma phase
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• Soft-wall model 1 : Karch, Katz, Son, Stephanov
A dilaton is introduced, Metrics are the same.
• Soft-wall model 2 : Andreev,Zakharov;Kajantie
modify string frame metric by a conformal factor
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• Free energy
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Td with deformed metric
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AdS/CFT and Lattice
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Summary
To assess the validity . At melting temperature of U satz
We calculated dissociation temperatures Td of heavy quarkonium states from holographic potential
The computed Td have remarkable features compariable with that from Lattice
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Thanks for your attention!