The analytic structure of the BFKL equation and reflection identities of harmonic sums at weight five
From MaRDI portal
Publication:5376997
DOI10.1142/S0217751X19500647zbMath1412.81173arXiv1903.06773WikidataQ127921184 ScholiaQ127921184MaRDI QIDQ5376997
Mohammad Joubat, Alexander Prygarin
Publication date: 21 May 2019
Published in: International Journal of Modern Physics A (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/1903.06773
Yang-Mills and other gauge theories in quantum field theory (81T13) Strong interaction, including quantum chromodynamics (81V05) Meromorphic functions of one complex variable (general theory) (30D30)
Related Items (2)
Pole decomposition of BFKL eigenvalue at zero conformal spin and the real part of digamma function ⋮ The analytic structure of the BFKL equation and reflection identities of harmonic sums at weight five
Uses Software
Cites Work
- Erratum to: ``Three-loop universal anomalous dimension of the Wilson operators in \(\mathcal N=4\) SUSY Yang-Mills model [Phys. Lett. B 595 (2004) 521]
- On a residual freedom of the next-to-leading BFKL eigenvalue in color adjoint representation in planar \( \mathcal{N}=4 \) SYM
- High-energy evolution to three loops
- BFKL eigenvalue and maximal alternation of harmonic sums
- Quantum Chromodynamics
- The analytic structure of the BFKL equation and reflection identities of harmonic sums at weight five
This page was built for publication: The analytic structure of the BFKL equation and reflection identities of harmonic sums at weight five
