DGLAP and BFKL equations in N=4 SYM: from weak to strong coupling

2019/08/14 by A. V. Kotikov, Kotikov, A. V., A. I. Onishchenko +1
Physics and Astronomy · #Black Holes and Theoretical Physics #Cosmology and Gravitation Theories #FOS: Physical sciences #High Energy Physics - Phenomenology (hep-ph) #High Energy Physics - Theory (hep-th) #Quantum Chromodynamics and Particle Interactions

paper · pdf · doi:10.48550/arxiv.1908.05113

openalex publication_date 2019/08/14 · openalex created_date 2019/08/22 · openalex updated_date 2026/07/28

Abstract

DGLAP and BFKL equations are among the cornestones of the contemporary QCD. Moreover, they also played an important role in the recent studies of integrability structure of N=4 SYM. Here, we review the results obtained along this way together with a brief account of approaches and methods used.

Citations

• An exact slope for AdS/CFT
• DGLAP and BFKL evolution equations in the N=4 supersymmetric gauge theory
• Long-range psu(2,2|4) Bethe ansätze for gauge theory and strings
• The dilatation operator of conformal super-Yang–Mills theory
• Analytic continuation of the Mellin moments of deep inelastic structure functions
• Scaling dimensions at small spin in N=4 SYM theory

Related

• DGLAP and BFKL evolution equations in the N=4 supersymmetric gauge theory
• BFKL pomeron in the next-to-next-to-leading approximation in the planar N=4 SYM theory
• Supersymmetric 4d gauge theories and Integrability
• DGLAP-BFKL duality from QCD to quantum computers
• Pomeron in the N=4 SYM