Handbook of perturbative QCD

G Sterman, J Smith, JC Collins, J Whitmore… - Reviews of Modern …, 1995 - APS
The elements, theoretical basis, and experimental status of perturbative quantum
chromodynamics are presented. Relevant field-theoretic methods are introduced at a …

The SAGEX review on scattering amplitudes Chapter 4: Multi-loop Feynman integrals

J Blümlein, C Schneider - Journal of Physics A: Mathematical and …, 2022 - iopscience.iop.org
The analytic integration and simplification of multi-loop Feynman integrals to special
functions and constants plays an important role to perform higher order perturbative …

[HTML][HTML] The three-loop unpolarized and polarized non-singlet anomalous dimensions from off shell operator matrix elements

J Blümlein, P Marquard, C Schneider, K Schönwald - Nuclear Physics B, 2021 - Elsevier
We calculate the unpolarized and polarized three–loop anomalous dimensions and splitting
functions P NS+, P NS− and P NS s in QCD in the MS‾ scheme by using the traditional …

The three-loop polarized singlet anomalous dimensions from off-shell operator matrix elements

J Blümlein, P Marquard, C Schneider… - Journal of high energy …, 2022 - Springer
A bstract Future high luminosity polarized deep-inelastic scattering experiments will improve
both the knowledge of the spin sub-structure of the nucleons and contribute further to the …

[HTML][HTML] The 3-loop non-singlet heavy flavor contributions and anomalous dimensions for the structure function F2 (x, Q2) and transversity

J Ablinger, A Behring, J Blümlein, A De Freitas… - Nuclear Physics B, 2014 - Elsevier
We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor
contributions to the structure function F 2 (x, Q 2) in the asymptotic region Q 2≫ m 2 and the …

[HTML][HTML] O (αs2) polarized heavy flavor corrections to deep-inelastic scattering at Q2≫ m2

I Bierenbaum, J Blümlein, A De Freitas, A Goedicke… - Nuclear Physics B, 2023 - Elsevier
We calculate the quarkonic O (α s 2) massive operator matrix elements Δ AQ g (N), Δ AQ q
PS (N) and Δ A qq, Q NS (N) for the twist–2 operators and the associated heavy flavor …

[HTML][HTML] The transition matrix element Agq (N) of the variable flavor number scheme at O (αs3)

J Ablinger, J Blümlein, A De Freitas, A Hasselhuhn… - Nuclear Physics B, 2014 - Elsevier
We calculate the massive unpolarized operator matrix element A gq (3)(N) to 3-loop order in
Quantum Chromodynamics at general values of the Mellin variable N. This is the first …

Analytic computing methods for precision calculations in quantum field theory

J Blümlein, C Schneider - International Journal of Modern Physics A, 2018 - World Scientific
An overview is presented on the current status of main mathematical computation methods
for the multiloop corrections to single-scale observables in quantum field theory and the …

[HTML][HTML] The polarized transition matrix element Agq (N) of the variable flavor number scheme at O (αs3)

A Behring, J Blümlein, A De Freitas, A von Manteuffel… - Nuclear Physics B, 2021 - Elsevier
We calculate the polarized massive operator matrix element A gq (3)(N) to 3-loop order in
Quantum Chromodynamics analytically at general values of the Mellin variable N both in the …

Two-loop massive operator matrix elements for unpolarized heavy flavor production to O (ϵ)

I Bierenbaum, J Blümlein, S Klein, C Schneider - Nuclear physics B, 2008 - Elsevier
We calculate the O (αs2) massive operator matrix elements for the twist-2 operators, which
contribute to the heavy flavor Wilson coefficients in unpolarized deeply inelastic scattering in …