Evolution of structure functions at NLO without PDFs

We formulate the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) evolution of the Deep Inelastic Scattering (DIS) structure functions $F_2$ and $F_{\rm L}$ at next to leading order in $\alpha_s$ (NLO) directly in terms of the structure functions rather than parton distributions (PDFs). We call this the physical basis approach. In practice, we first express the NLO quark singlet and gluon PDFs in terms of the structure functions $F_2$ and $F_{\rm L}$ in momentum space. Employing these expressions in the DGLAP evolution, we arrive at the evolution equations for $F_2$ and $F_{\rm L}$ in the physical basis. We demonstrate how one is free from defining a factorization scale and scheme when using the physical basis evolution equations. We also discuss the process of applying the NLO physical basis to global analysis of LHC cross sections.

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Publication Details

Published
2024-12-27
DOI
https://doi.org/10.22323/1.469.0030
Primary Topic
Reservoir Engineering and Simulation Methods
Type
article
Field-Weighted Citation Impact
0.00

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article

Evolution of structure functions at NLO without PDFs

Heikki Mäntysaari, Mirja Tevio, Hannu Paukkunen, T. Lappi
Reservoir Engineering and Simulation Methods
article

Evolution of structure functions at NLO without PDFs

Heikki Mäntysaari, Mirja Tevio, Hannu Paukkunen, T. Lappi
article en

Abstract

We formulate the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) evolution of the Deep Inelastic Scattering (DIS) structure functions $F_2$ and $F_{\rm L}$ at next to leading order in $\alpha_s$ (NLO) directly in terms of the structure functions rather than parton distributions (PDFs). We call this the physical basis approach. In practice, we first express the NLO quark singlet and gluon PDFs in terms of the structure functions $F_2$ and $F_{\rm L}$ in momentum space. Employing these expressions in the DGLAP evolution, we arrive at the evolution equations for $F_2$ and $F_{\rm L}$ in the physical basis. We demonstrate how one is free from defining a factorization scale and scheme when using the physical basis evolution equations. We also discuss the process of applying the NLO physical basis to global analysis of LHC cross sections.

Strong, European Commission
Openalex Percentile: Top 67%
Reservoir Engineering and Simulation Methods
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Evolution of structure functions at NLO without PDFs — Heikki Mäntysaari, Mirja Tevio, et al. · (2024) | TGRS Research Map | TGRS