13.06.2014 Views

Gauge/gravity duality: an overview Z. Bajnok

Gauge/gravity duality: an overview Z. Bajnok

Gauge/gravity duality: an overview Z. Bajnok

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

R 2<br />

α ′<br />

II B superstring on AdS 5 × S 5<br />

4D<br />

Minkowski<br />

space<br />

5D<br />

<strong>an</strong>ti de Sitter<br />

space<br />

AdS/CFT correspondence (Maldacena 1998)<br />

5D sphere<br />

≡<br />

space<br />

time<br />

extra dimension<br />

( )<br />

∂a X M ∂ a X M + ∂ a Y M ∂ a Y M + . . .<br />

∑ 6<br />

1 Y i 2 = R 2 − + + + +− = −R 2<br />

∫ dτdσ<br />

4π<br />

Couplings: √ λ = R2<br />

α ′ , g s = λ N → 0<br />

2D QFT<br />

String energy levels: E(λ)<br />

E(λ) = E(∞) + √ E 1<br />

+ E 2<br />

λ λ + . . .<br />

Dictionary<br />

2<br />

g 2 Y M<br />

strong↔weak<br />

⇓<br />

N = 4 D=4 SU(N) SYM<br />

∫ d 4 xTr [ − 1 4 F 2 − 1 2 (DΦ)2 + iΨD/ Ψ + V ]<br />

V (Φ, Ψ) = 1 4 [Φ, Φ]2 + Ψ[Φ, Ψ]<br />

P SU(2,2|4)<br />

β = 0 superconformal<br />

SO(5)×SO(1,4)<br />

gaugeinvari<strong>an</strong>ts:O = Tr(Φ 2 ), det( )<br />

λ = gY 2 MN , N → ∞ pl<strong>an</strong>ar limit<br />

〈O n (x)O m (0)〉 = δ nm<br />

|x| 2∆ n(λ)<br />

Anomalous dim ∆(λ)<br />

∆(λ) = ∆(0) + λ∆ 1 + λ 2 ∆ 2 + . . .<br />

2D integrable QFT<br />

√<br />

spectrum: Q = 1, 2, . . . , ∞ dispersion: ɛ Q (p) = Q 2 + λ π 2 sin2 p<br />

2<br />

Exact scattering matrix: S Q1 Q 2<br />

(p 1 , p 2 , λ)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!