Unpolarized GPDs at small x and non-zero skewness

We study the small-$x$ asymptotics of unpolarized generalized parton distributions (GPDs) and generalized transverse momentum distributions (GTMDs). Unlike the previous works in the literature, we consider the case of non-zero (but small) skewness while allowing for non-linear contributions to the evolution equations. We show that unpolarized GPDs and GTMDs at small $x$ are related to the eikonal dipole amplitude $N$, whose small-$x$ evolution is given by the BK/JIMWLK evolution equations, and to the odderon amplitude $\cal O$, whose evolution is also known in the literature. We show that the effect of non-zero skewness $ξ\neq 0$ is to modify the value of the evolution parameter (rapidity) in the arguments for the dipole amplitudes $N$ and $\cal O$ from $Y = \ln (1/x)$ to $Y = \ln \min \left\{ 1/|x| , 1/|ξ| \right\}$.

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Publication Details

Journal
Physics Letters B
Published
2026-04-22
DOI
https://doi.org/10.1016/j.physletb.2026.140470
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
0.00

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article

Unpolarized GPDs at small x and non-zero skewness

H. K. Sun, M. Gabriel Santiago, Yuri V. Kovchegov
Physics Letters B
Particle physics theoretical and experimental studies
article

Unpolarized GPDs at small x and non-zero skewness

H. K. Sun, M. Gabriel Santiago, Yuri V. Kovchegov
article en

Abstract

We study the small-$x$ asymptotics of unpolarized generalized parton distributions (GPDs) and generalized transverse momentum distributions (GTMDs). Unlike the previous works in the literature, we consider the case of non-zero (but small) skewness while allowing for non-linear contributions to the evolution equations. We show that unpolarized GPDs and GTMDs at small $x$ are related to the eikonal dipole amplitude $N$, whose small-$x$ evolution is given by the BK/JIMWLK evolution equations, and to the odderon amplitude $\cal O$, whose evolution is also known in the literature. We show that the effect of non-zero skewness $ξ\neq 0$ is to modify the value of the evolution parameter (rapidity) in the arguments for the dipole amplitudes $N$ and $\cal O$ from $Y = \ln (1/x)$ to $Y = \ln \min \left\{ 1/|x| , 1/|ξ| \right\}$.

Physics Letters BVol. 877
U.S. Department of Energy, Office of Science, Nuclear Physics, Thomas Jefferson National Accelerator Facility
Openalex Percentile: Top 96%
Particle physics theoretical and experimental studies
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