based on collaboration with s.nakamura, ys.seo, p.yogendran (hanyang,cquest)
DESCRIPTION
Some Issues in AdS/QCD. Sang-Jin Sin (Hanyang Univ.) 2007.11.30 @HYU. Based on collaboration with S.Nakamura, YS.Seo, P.Yogendran (Hanyang,cquest) BH.Lee, YM.Kim, CY.Park (Cquest, KIAS) E.Shuryak, I.Zahed, KY.Kim (Stony Brook). String Theory and Hadron physics. - PowerPoint PPT PresentationTRANSCRIPT
Based on collaboration withS.Nakamura, YS.Seo, P.Yogendran (Hanyang,cquest)
BH.Lee, YM.Kim, CY.Park (Cquest, KIAS)E.Shuryak, I.Zahed, KY.Kim (Stony Brook)
Some Issues in AdS/QCD
Sang-Jin Sin (Hanyang Univ.)2007.11.30 @HYU
String Theory and Hadron physics1. Invented as a Hadron theory (1GeV) 2. Became theory of gravity (plank scale)3. back to Hadron theory with AdS/CFT4. Key idea: D-brane ,
Open-Closed string duality(gauge/gravity) 5. Decoupling of Plank scale: New scale
=AdS radius t`Hooft coupling of gauge theory.
D-brane Open string gauge theory Closed string gravity D-brane=Membrane like closed string
solitonwhose vibration is restricted as open string vibration.
Quarks, baryons, chemical potentials
mu=A at infinity
Nf
Nc
D5
D3
F1
Quark=string connecting color & flavor branes
Chemical potential= tail of electricpotential
Baryon vertex
A few questions in RHIC//AdS1. Jet quenching (with I. Zahed 2004)2. Elliptic Flow (with S.Nakamura & SP.
Kim,06)3. Cooling and Expansion Rate (Shuryak &
Zahed,05)4. Calculation of dissipation in expanding
Fireball (with KY.Kim & Zahed, 07)5. Dense matter effect and Phase diagram
(with Nakamura, Seo, Yogendran, 06)6. Rapid thermalization
In the rest of this talk I will pick up one issue and give some
details .
Phase diagram in Temperature-Density plane
Back reaction of geometry to the dense matter is essential. With and only with BR, Phase diagram closes
Deconfinement Phase Transition 1. Without Matter: Hawking Page Transition
between Two competing geometries: AdS with IR cutoff (Low T) & AdS BH (High T)
2. what if there is baryon chage?
Problem in Probe brane description Large Nc and finite Nf: little effect of baryon/quark density in phase
transition and P.D is OPEN
Nf T
density
confinement
Nf/Nc=finite
Origin of the problem Nf/Nc ~ 1 in QCD.
Since Nc has to be large for AdS/CFT, so is the Nf. Then gravity back reaction is not an option but an essential.
back reaction closes phase diagram.
Baryon is not adjoint Rep. not a Bulk Field.
Chemical potential in 4d is a constant A0. Therefore mu= Tail of BRANE-FIELD A0.
(Kim-Sin-Zahed : hep-th/0608046) Horigome-Tanii (hep-th/0608198)
Use eq. of Motion for A_0
mu=
A a
t infinity
a brane U(1) charge
If Brane is Filling entire AdS 5 brane charge= bulk charge.
Since there is a unique way a U(1) charge can couple to the metric, U(1)_B charge must be related to the charge parameter in RN black hole.
Chamblin et.al hep-th/9902170:
Q identified as R charge
Bulk field A sourced by Adjoint representation
Bulk=Brane R charge and Q play the same role
Fixed chemical potential (grand canonical)
• Fixed charge (Canonical) : add a surface term or Legendre transform
• grand canonical v.s Canonical
Introducing hard wallHawking-Page Transition (Herzog)
High temperature: charged ads BH Low temperature: AdS with charges at the wall
for fixed charge case Treat the grand canonical as Legendre Tr.
Of canonical case.