The two-mass contribution to the three-loop gluonic operator matrix element \(A_{g g, Q}^{(3)}\)
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Publication:721637
DOI10.1016/j.nuclphysb.2018.04.023zbMath1391.81202arXiv1804.02226OpenAlexW2796071844MaRDI QIDQ721637
A. Goedicke, Johannes Blümlein, K. Schönwald, Carsten Schneider, Abilio De Freitas, Jakob Ablinger
Publication date: 19 July 2018
Published in: Nuclear Physics. B (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/1804.02226
Nuclear physics (81V35) Strong interaction, including quantum chromodynamics (81V05) Feynman diagrams (81T18)
Related Items (15)
The first-order factorizable contributions to the three-loop massive operator matrix elements \(A_{Qg}^{(3)}\) and \(\Delta A_{Qg}^{(3)}\) ⋮ The massless three-loop Wilson coefficients for the deep-inelastic structure functions \(F_2\), \(F_L\), \(xF_3\) and \(g_1\) ⋮ The inverse Mellin transform via analytic continuation ⋮ Minimal representations and algebraic relations for single nested products ⋮ The three-loop polarized pure singlet operator matrix element with two different masses ⋮ The three-loop single mass polarized pure singlet operator matrix element ⋮ 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 \(e^+ e^- \to \gamma^\ast / Z_0^\ast \) ⋮ The polarized transition matrix element \(A_{gq}(N)\) of the variable flavor number scheme at \(O(\alpha_s^3)\) ⋮ On rational and hypergeometric solutions of linear ordinary difference equations in \(\Pi\Sigma^\ast\)-field extensions ⋮ The unpolarized two-loop massive pure singlet Wilson coefficients for deep-inelastic scattering ⋮ Large Scale Analytic Calculations in Quantum Field Theories ⋮ Analytic Integration Methods in Quantum Field Theory: An Introduction ⋮ Term Algebras, Canonical Representations and Difference Ring Theory for Symbolic Summation ⋮ The SAGEX review on scattering amplitudes Chapter 4: Multi-loop Feynman integrals
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