The polarized two-loop massive pure singlet Wilson coefficient for deep-inelastic scattering

DOI10.1016/j.nuclphysb.2019.114736zbMath1435.81226arXiv1904.08911OpenAlexW2921055758WikidataQ127353104 ScholiaQ127353104MaRDI QIDQ2186353

K. Schönwald, Johannes Blümlein, Clemens G. Raab

Publication date: 9 June 2020

Published in: Nuclear Physics. B (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/1904.08911

Mathematics Subject Classification ID

Feynman integrals and graphs; applications of algebraic topology and algebraic geometry (81Q30) Finite-dimensional groups and algebras motivated by physics and their representations (81R05) (2)-body potential quantum scattering theory (81U05) Elliptic functions and integrals (33E05)

Related Items (9)

The two-loop massless off-shell QCD operator matrix elements to finite terms ⋮ The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements ⋮ The massless three-loop Wilson coefficients for the deep-inelastic structure functions \(F_2\), \(F_L\), \(xF_3\) and \(g_1\) ⋮ \(O(\alpha_s^2)\) polarized heavy flavor corrections to deep-inelastic scattering at \(Q^2 \gg m^2\) ⋮ The three-loop polarized pure singlet operator matrix element with two different masses ⋮ The two-mass contribution to the three-loop polarized gluonic operator matrix element \(A_{gg, Q}^{(3)}\) ⋮ The \(O(\alpha^2)\) initial state QED corrections to \(e^+ e^- \to \gamma^\ast / Z_0^\ast \) ⋮ Nested Integrals and Rationalizing Transformations ⋮ The SAGEX review on scattering amplitudes Chapter 4: Multi-loop Feynman integrals

Uses Software

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