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Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and...

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N=4 Supersymmetric Yang-Mills Theory The action: Field content:
23
Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira
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Page 1: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

Integrability for the Full Spectrum of Planar AdS/CFT Nikolay GromovDESY/HU/PNPIV.Kazakov and P.Vieira

Page 2: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

Motivation

Spectrum of an interacting field theory is a funny problem by itself

Some quantities are shared with realistic QCD

We can test string/gauge duality

Page 3: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

N=4 Supersymmetric Yang-Mills Theory

The action:

Field content:

Page 4: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

YM: Local operators and spin chains

- Dilatation operator – integrable Hamiltonian

Page 5: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

The spectrumGround state:

Excited states (magnons):

Page 6: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

periodicity condition:

momentumscattering phase shifts

periodicity of wave function

©Zarembo

Page 7: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

7

2) Get eigenvalues

1) Solve polynomial equation

YM: One-loop- Integrable Hamiltonian

LepatovFaddeev, KorchemskyMinahan , Zarembo

Page 8: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

8

Numerical Solution

Till Bargheer, Niklas Beisert, N. G.

Page 9: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

String theory

Page 10: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

(type IIB super) string theory in AdS5xS5 x

is dual to a 4 dimensional conformal field theory (N=4 SYM)

Local operators String states

Maldacena

AdS/CFT Duality

Anomalous dimensions Spectrum

Page 11: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

x

String tension `t Hooft coupling

String coupling Number of colors

AdS/CFT Duality

Summetry:

Page 12: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

Beisert, Staudacher;Beisert,Eden,Staudacher

Bethe equations

Page 13: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

Vacuum

I.e. from the asymptotical spectrum (R=\infty) we can compute the Ground state energy for ANY finite volume!

Page 14: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

SO(4)

Symmetry:

Анзац Бетэ:Zamolodchikov x2Faddeev, Reshetikhin

Page 15: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

Ground state from ABAThe typical configuration of roots

isWe define:

Saddle point equation:

Page 16: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

Above ground stateDorey, Totteo,Bazhanov

Page 17: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

Spectrum of SO(4)

Page 18: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

AdS/CFT GeneralizationN.G., Kazakov, Vieira

Page 19: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

Large L limit

Use Hirota equation:

Page 20: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

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S-matrix

Obeys Yang-Baxter:

Then (see lectures of Faddeev hep-th/9605187 ):

SU(2|2) invariant tensor with 4 fundamental indeses

The eigevalues solves hirota!

Page 21: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

Konishi operator

For weak coupling constant:

The simplest operator

In agreement with perturbation theory!!4-loops!

Kotikov, Lipatov, Rej, Staudacher and VelizhaninSieg, TorrielliJanik, Bojnok, N.G., Kazakov, Vieira

Page 22: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

CP3xAdS4 / N=6 Chern-Simons

N.G., Kazakov, Vieira

Aharony, Bergman, Jafferis and Maldacena

Page 23: Integrability for the Full Spectrum of Planar AdS/CFT Nikolay Gromov DESY/HU/PNPI V.Kazakov and P.Vieira.

Conclusions

We can go below BAE nowIntegrability allows to predict

very complicated perturbative calculations

It is possible to compute some quantities for arbitrary coupling

QCD BFKL could be checked


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