M. Saragnese

activity

20192024

most citedThe N

^{3}

LO Scheme-invariant QCD Evolution of the Non-singlet Structure Functions \boldmath

F_{2}^{NS} (x, Q^{2})

and

g_{1}^{NS} (x, Q^{2})

30 citations · 95 across the 6 of their papers we have counts for

collaborators

Showing 2021Show all

4 papers · 1 filter

math-ph2021

Hypergeometric Structures in Feynman Integrals

J. Blümlein, M. Saragnese, C. Schneider

Hypergeometric structures in single and multiscale Feynman integrals emerge in a wide class of topologies. Using integration-by-parts relations, associated master or scalar integra…

hep-ph2021

New 2- and 3-loop heavy flavor corrections to unpolarized and polarized deep-inelastic scattering

J. Ablinger, J. Blümlein, A. De Freitas +3

A survey is given on the new 2- and 3-loop results for the heavy flavor contributions to deep-inelastic scattering in the unpolarized and the polarized case. We also discuss relate…

hep-ph2021★ 30 cited

The N $^{3}$ LO Scheme-invariant QCD Evolution of the Non-singlet Structure Functions \boldmath $F_{2}^{NS} (x, Q^{2})$ and $g_{1}^{NS} (x, Q^{2})$

J. Blümlein, M. Saragnese

We present the scheme-invariant unpolarized and polarized flavor non-singlet evolution equation to N $^{3}$ LO for the structure functions $F_{2} (x, Q^{2})$ and $g_{1} (x, Q^{2})$ including the c…

hep-ph2021★ 21 cited

The Logarithmic Contributions to the Polarized and Operator Matrix Elements in Deeply Inelastic Scattering

J. Blümlein, A. De Freitas, M. Saragnese +2

We compute the logarithmic contributions to the polarized massive Wilson coefficients for deep-inelastic scattering in the asymptotic region $Q^{2} ≫ m^{2}$ to 3-loop order in the fi…

Hypergeometric Structures in Feynman Integrals

New 2- and 3-loop heavy flavor corrections to unpolarized and polarized deep-inelastic scattering

The N3LO Scheme-invariant QCD Evolution of the Non-singlet Structure Functions \boldmath F2NS​(x,Q2) and g1NS​(x,Q2)

The Logarithmic Contributions to the Polarized and Operator Matrix Elements in Deeply Inelastic Scattering

The N $^{3}$ LO Scheme-invariant QCD Evolution of the Non-singlet Structure Functions \boldmath $F_{2}^{NS} (x, Q^{2})$ and $g_{1}^{NS} (x, Q^{2})$