The two-mass contribution to the three-loop polarized gluonic operator matrix element \(A_{gg, Q}^{(3)}\)

DOI10.1016/j.nuclphysb.2020.115059zbMath1473.81191arXiv2004.08916OpenAlexW4242541884MaRDI QIDQ2230258

Johannes Blümlein, K. Schönwald, Carsten Schneider, Jakob Ablinger, A. Goedicke, M. Saragnese, Abilio De Freitas

Publication date: 17 September 2021

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

Full work available at URL: https://arxiv.org/abs/2004.08916

Mathematics Subject Classification ID

Nuclear physics (81V35) Strong interaction, including quantum chromodynamics (81V05) Inelastic and multichannel quantum scattering (81U35) Operator matrices (47A08) Effective quantum field theories (81T12)

Related Items

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 polarized transition matrix element \(A_{gq}(N)\) of the variable flavor number scheme at \(O(\alpha_s^3)\) ⋮ Collider physics at the precision frontier ⋮ The three-loop polarized singlet anomalous dimensions from off-shell operator matrix elements ⋮ Differential Equations and Feynman Integrals ⋮ The SAGEX review on scattering amplitudes Chapter 4: Multi-loop Feynman integrals

Uses Software

• FORM
• HarmonicSums
• Axodraw

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