2013/01/31 by A. V. Kotikov, L. N. Lipatov, L.N. Lipatov · 1 citation
Mathematics · Physics and Astronomy · #Black Holes and Theoretical Physics #Combinatorics #Dimension (graph theory) #Geometry #Inverse #Mathematical physics #Mathematics #Order (exchange) #Particle physics #Particle physics theoretical and experimental studies #Perturbation theory (quantum mechanics) #Physics #Pomeron #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #hep-th
paper · pdf · doi:10.1016/j.nuclphysb.2013.06.018
18 pages, 1 figure, fixed some typos
openalex publication_date 2013/07/01 · arxiv created 2014/01/03 · arxiv updated 2015/06/12 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We find the BFKL Pomeron intercept at N=4 supersymmetric gauge theory in the form of the inverse coupling expansion j0=2−2λ−1/2−λ−1+1/4λ−3/2+2(1+3ζ3)λ−2+O(λ−5/2) with the use of the AdS/CFT correspondence in terms of string energies calculated recently. The corresponding slope γ′(2) of the anomalous dimension calculated directly up to the fifth order of perturbation theory turns out to be in an agreement with the closed expression obtained from the recent Basso results.