2009
DOI: 10.1103/physrevlett.103.131601
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Exact Spectrum of Anomalous Dimensions of PlanarN=4Supersymmetric Yang-Mills Theory

Abstract: We present a set of functional equations defining the anomalous dimensions of arbitrary local single trace operators in planar N = 4 SYM theory. It takes the form of a Y-system based on the integrability of the dual superstring σ-model on the AdS5 × S 5 background. This Y-system passes some very important tests: it incorporates the full asymptotic Bethe ansatz at large length of operator L, including the dressing factor, and it confirms all recently found wrapping corrections. The recently proposed AdS4/CF T3 … Show more

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Cited by 309 publications
(283 citation statements)
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“…Using the so-called BES equation [8] the cusp anomalous dimension f (λ) was thoroughly studied both in the weak [8,11] and strong coupling regime [9,10,11]. Furthermore, all contributions to the exact in S anomalous dimension (2) which are free from wrapping effects can, in principle, be calculated [12,15] by using a linear integral equation previously derived in [14] 2 .…”
Section: Introductionmentioning
confidence: 99%
“…Using the so-called BES equation [8] the cusp anomalous dimension f (λ) was thoroughly studied both in the weak [8,11] and strong coupling regime [9,10,11]. Furthermore, all contributions to the exact in S anomalous dimension (2) which are free from wrapping effects can, in principle, be calculated [12,15] by using a linear integral equation previously derived in [14] 2 .…”
Section: Introductionmentioning
confidence: 99%
“…In the next chapter, we are going to explain the significance of this simplification. We define then 104) where K + and K − contain the expansion on odd and even Bessel functions respectively. The "magic" formula of BES expresses the dressing kernel as…”
Section: The "Magic" Bes Formulamentioning
confidence: 99%
“…The increasing linearity of the plot as the lattice size increases is very consistent with a power law behavior in the infinite volume limit. In principle the slope of this line yields (twice) the scaling dimension of the Konishi operator and we are currently working hard to extract this scaling dimension as a function of the 't Hooft coupling to compare with results in the planar limit 57 and bounds from the conformal bootstrap approach. 56 Preliminary results obtained from a Monte Carlo renormalization group analysis are in agreement with perturbative calculations at weak coupling.…”
Section: N = 4 Supersymmetric Yang-mills Theorymentioning
confidence: 99%