Konishi:%20from%204%20loops%20to%20infinity - PowerPoint PPT Presentation

About This Presentation
Title:

Konishi:%20from%204%20loops%20to%20infinity

Description:

The problem of diagonalization of the huge matrix can be solved by Bethe ansatz ... Bianchi, Kovacs,Rossi, Stanev; Eden, Jarczak, Sokatchev,Stanev... – PowerPoint PPT presentation

Number of Views:49
Avg rating:3.0/5.0
Slides: 21
Provided by: hp26175
Category:

less

Transcript and Presenter's Notes

Title: Konishi:%20from%204%20loops%20to%20infinity


1
Konishi from 4 loops to infinity
Nikolay Gromov Based on works with V.Kazakov,
P.Vieira A.Kozak
Symposium on Theoretical and Mathematical
Physics July 3-8, 2009
2
AdS/CFT correspondence
AdS/CFT duality
String tension
t Hooft coupling
Anomalous dimensions spectrum of 2D integrable
field theories
Symmetry
3
Integrability in N4 SYM
N4 Super Yang-Mills
- Mixing matrix integrable Hamiltonian
Minahan, Zarembo 20022008
The problem of diagonalization of the huge matrix
can be solved by Bethe ansatz
4
Clasical integrability
Motion of the strin in AdS
Infinitely many Integrals of motion
5
Integrability in 2D
Operator corresponding to an integral of motion
Between in and out states
The outgoing momenta are constrained
The only solution
6
Factorization of S-matrix
Yang-Baxter equation
7
Asymptotic Spectrum
  • For spectral density we need finite volume
  • From periodicity of the wave function-Bethe
    equations

8
Bethe equations
Beisert, Staudacher Beisert, Hernandez,
Lopez Beisert,Eden,Staudacher Arutyunov, Frolov
9
Vacuum
,Matsubara, Zamolodchikov,
I.e. from the asymptotical spectrum (infinite R)
we can compute the Ground state energy for ANY
finite volume!
In our case the wick rotated theory is different
mirror theory
Ambjorn, Janik, Kristjansen Arutynov, Frolov
10
AdS/CFT bound states
Till Bargheer, Niklas Beisert, N. G.
11
AdS/CFT Y-system
N.G., Kazakov, Vieira
Bazhanov, Lukyanov, Zamolodchikov, P.Dorey,
Totteo
Destri de Vega, Bytsko ,Teschner.
12
Above ground state
Bazhanov, Lukyanov, Zamolodchikov, P.Dorey, Totteo
Inspiration 1 Analytical continuation
Inspiration 2 Integrable lattice models
Destri de Vega, Teschner
13
Large L limit or weak coupling
N.G., Kazakov, Vieira
Use Hirota equation
14
Hirota large L
The eigevalues solve Hirota! for rep
15
Explicitly
Instead of computing the transfer matrices
explicitly one can use
16
Konishi operator
The simplest operator
Bianchi, Kovacs,Rossi, Stanev Eden, Jarczak,
Sokatchev,Stanev
In agreement with perturbation theory!! 4-loops!
Kotikov, Lipatov, Rej, Staudacher and
Velizhanin Sieg, Torrielli Janik, Bojnok, N.G.,
Kazakov, Vieira
17
Integral form of Y-system for exitations
Bombardelli, Fioravanti, Tateo N.G., Kazakov,
Vieira Arutynov, Frolov
18
Exact BAE
  • From mirror to physical

Precision is excellent!!!
19
Konishi from weak to strong
Fit
From string side Roiban,Tseytlin
20
Numerical results
  • 20 computers 4 nights
  • Emergence of integers a miracle
  • Exact BAE modified by phase

Porto university Wolfram
21
Comparison with Roiban and Tseytlin
22
Conclutions
  • Y-system is proven to be a computational tool
  • We reproduced several leading terms at strong
    coupling for a simple operator
  • Any sl2 operator could be computed readily for
    any g
  • Generalization to other sectors to be done
  • Analytical results coming soon?
  • Other AdS/CFTs?

N.G., Kazakov, Vieira
Write a Comment
User Comments (0)
About PowerShow.com