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Quantum Corrections to the Weizsäcker--Williams Distribution Function as Small x

A. Ayala, J. Jalilian--Marian, L. Mclerran, R. Venugopalan

TL;DR

The authors compute quantum corrections to the small-$x$ gluon distribution in a non-Abelian Weizsäcker–Williams background field generated by valence quarks in a large nucleus, deriving results valid to all orders in $α_s μ$. They extract the leading $ abla(1/x)$-type logarithms and show that loop corrections to the background field merely renormalize the coupling $g$ (and the background field) rather than introduce new singular terms. The analysis reveals that the effective perturbative expansion is governed by $α_s \ln(1/x)$, indicating the necessity of resumming leading logs at very small $x$. The central results are encapsulated in a general expression for quantum corrections to the distribution, with explicit perturbative corrections and a clear separation between fluctuation-induced effects and background renormalization.

Abstract

We compute the quantum corrections to the gluon distribution function in the background of a non--Abelian Weizsäcker--Williams field. These corrections are valid to all orders in the effective coupling $α_s μ$, where $μ^2$ denotes the average valence quark color charge squared per unit area. We find $\ln(1/x)$ logarithmic corrections to the classical gluon distribution function. The one loop corrections to the classical Weizsäcker-Williams field do not contribute to these singular terms in the distribution function. Their effect is to cause the running of $α_s$.

Quantum Corrections to the Weizsäcker--Williams Distribution Function as Small x

TL;DR

The authors compute quantum corrections to the small- gluon distribution in a non-Abelian Weizsäcker–Williams background field generated by valence quarks in a large nucleus, deriving results valid to all orders in . They extract the leading -type logarithms and show that loop corrections to the background field merely renormalize the coupling (and the background field) rather than introduce new singular terms. The analysis reveals that the effective perturbative expansion is governed by , indicating the necessity of resumming leading logs at very small . The central results are encapsulated in a general expression for quantum corrections to the distribution, with explicit perturbative corrections and a clear separation between fluctuation-induced effects and background renormalization.

Abstract

We compute the quantum corrections to the gluon distribution function in the background of a non--Abelian Weizsäcker--Williams field. These corrections are valid to all orders in the effective coupling , where denotes the average valence quark color charge squared per unit area. We find logarithmic corrections to the classical gluon distribution function. The one loop corrections to the classical Weizsäcker-Williams field do not contribute to these singular terms in the distribution function. Their effect is to cause the running of .

Paper Structure

This paper contains 7 sections, 119 equations.