English

Pomeron in the N=4 SYM

High Energy Physics - Theory 2015-02-26 v2

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=22λ1/2λ1+1/4λ3/2+2(3ζ3+1)λ2+(18ζ3+361/64)λ5/2+(39ζ3+447/32)λ3+O(λ7/2)j_0=2-2\lambda^{-1/2}-\lambda^{-1} + 1/4 \, \lambda^{-3/2} + 2(3\zeta_3+1) \, \lambda^{-2} +(18\zeta_3+361/64) \, \lambda^{-5/2} + (39\zeta_3+447/32) \, \lambda^{-3} + O(\lambda^{-7/2}) which has been calculated in [1]-[5] with the use of the AdS/CFT correspondence.

Keywords

Cite

@article{arxiv.1412.6536,
  title  = {Pomeron in the N=4 SYM},
  author = {A. V. Kotikov},
  journal= {arXiv preprint arXiv:1412.6536},
  year   = {2015}
}

Comments

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

R2 v1 2026-06-22T07:38:49.476Z