The single-mass variable flavor number scheme at three-loop order

A bstract The matching relations in the unpolarized and polarized variable flavor number scheme at three-loop order are presented in the single-mass case. They describe the process of massive quarks becoming light at large virtualities Q 2 . In this framework, heavy-quark parton distributions can be defined. Numerical results are presented on the matching relations in the case of the single-mass variable flavor number scheme for the light parton, charm and bottom quark distributions. These relations are process independent. In the polarized case we generally work in the Larin scheme. To two-loop order we present the polarized massive OMEs also in the $$ \overline{\textrm{MS}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mi>MS</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> scheme. Fast numerical codes for the single-mass massive operator matrix elements are provided.

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Publication Details

Journal
Journal of High Energy Physics
Published
2026-03-26
DOI
https://doi.org/10.1007/jhep03(2026)248
Primary Topic
Particle physics theoretical and experimental studies
Type
article
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article

The single-mass variable flavor number scheme at three-loop order

Jakob Ablinger, Kay Schönwald, Arnd Behring, Abilio De Freitas et al.
Journal of High Energy Physics
Particle physics theoretical and experimental studies
article

The single-mass variable flavor number scheme at three-loop order

Jakob Ablinger, Kay Schönwald, Arnd Behring, Abilio De Freitas, C. Schneider, A. von Manteuffel, J. Blümlein
article en

Abstract

A bstract The matching relations in the unpolarized and polarized variable flavor number scheme at three-loop order are presented in the single-mass case. They describe the process of massive quarks becoming light at large virtualities Q 2 . In this framework, heavy-quark parton distributions can be defined. Numerical results are presented on the matching relations in the case of the single-mass variable flavor number scheme for the light parton, charm and bottom quark distributions. These relations are process independent. In the polarized case we generally work in the Larin scheme. To two-loop order we present the polarized massive OMEs also in the $$ \overline{\textrm{MS}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mi>MS</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> scheme. Fast numerical codes for the single-mass massive operator matrix elements are provided.

Journal of High Energy PhysicsVol. 2026(3)
Johannes Kepler University of Linz (AT), University of Zurich (CH), Deutsches Elektronen-Synchrotron DESY (DE), Max Planck Institute for Physics (DE), Institut für Technische und Angewandte Physik (Germany) (DE), University of Regensburg (DE), European Organization for Nuclear Research (CH)
Openalex Percentile: Top 4%
Particle physics theoretical and experimental studies
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The single-mass variable flavor number scheme at three-loop order — Jakob Ablinger, Kay Schönwald, et al. · Journal of High Energy Physics (2026) | TGRS Research Map | TGRS