Pomeron in the N=4 SYM

2014/12/19 by A. V. Kotikov, Kotikov, A. V.
Physics and Astronomy · #Black Holes and Theoretical Physics #FOS: Physical sciences #High Energy Physics - Theory (hep-th) #Particle physics theoretical and experimental studies #Quantum Chromodynamics and Particle Interactions #hep-th

paper · pdf · doi:10.48550/arxiv.1412.6536

5 pages, 1 figure, talk given on the international Workshop "Hadron Structure and QCD" (HSQCD'2014), June 30 - July 4, Gatchina, 2014; one reference was added in the second version

openalex publication_date 2014/12/19 · arxiv created 2015/02/25 · arxiv updated 2015/02/26 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28

Abstract

We review the result for the BFKL Pomeron intercept at N=4 Supersymmetric Yang-Mills model in the form of the inverse coupling expansion j₀=2-2λ^-1/2-λ^-1 + 1/4 λ^-3/2 + 2(3ζ₃+1) λ^-2 +(18ζ₃+361/64) λ^-5/2 + (39ζ₃+447/32) λ^-3 + O(λ^-7/2) which has been calculated in [1]-[5] with the use of the AdS/CFT correspondence.

Related

• BFKL pomeron in the next-to-next-to-leading approximation in the planar N=4 SYM theory
• BFKL Pomeron and Bern-Dixon-Smirnov amplitudes in N=4 SUSY
• NNNLLA BFKL pomeron eigenvalue in the planar N=4 SYM theory
• Field theory insight from the AdS/CFT correspondence
• N=4 supersymmetric Yang-Mills theory and the AdS/SCFT correspondence