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Non-Abelian Weizsacker-Williams field and a two-dimensional effective color charge density for a very large nucleus

Yuri V. Kovchegov

TL;DR

The paper derives the classical non-Abelian Weizsäcker-Williams field for a very large ultra-relativistic nucleus and constructs the corresponding two-dimensional color charge density ρ_perp within the McLerran-Venugopalan framework. By evaluating density correlators, it shows that ρ_perp has a Gaussian distribution with a spatially dependent variance μ^2(x), thereby validating the MV averaging prescription for small-x observables and linking μ^2 to the nucleus geometry. The results yield an explicit expression for μ^2(x) and demonstrate that odd-density correlators vanish while even correlators factorize, implying a consistent Gaussian functional weight for all observables of the form O_ρ. This provides a solid field-theoretic basis for calculating Wilson-loop–type observables and gluon distributions in very large nuclei at small x.

Abstract

We consider a very large ultra-relativistic nucleus. Assuming a simple model of the nucleus and weak coupling we find a classical solution for the gluon field of the nucleus and construct the two-dimensional color charge density for McLerran-Venugopalan model out of it. We prove that the density of states distribution, as a function of color charge density, is Gaussian, confirming the assumption made by McLerran and Venugopalan.

Non-Abelian Weizsacker-Williams field and a two-dimensional effective color charge density for a very large nucleus

TL;DR

The paper derives the classical non-Abelian Weizsäcker-Williams field for a very large ultra-relativistic nucleus and constructs the corresponding two-dimensional color charge density ρ_perp within the McLerran-Venugopalan framework. By evaluating density correlators, it shows that ρ_perp has a Gaussian distribution with a spatially dependent variance μ^2(x), thereby validating the MV averaging prescription for small-x observables and linking μ^2 to the nucleus geometry. The results yield an explicit expression for μ^2(x) and demonstrate that odd-density correlators vanish while even correlators factorize, implying a consistent Gaussian functional weight for all observables of the form O_ρ. This provides a solid field-theoretic basis for calculating Wilson-loop–type observables and gluon distributions in very large nuclei at small x.

Abstract

We consider a very large ultra-relativistic nucleus. Assuming a simple model of the nucleus and weak coupling we find a classical solution for the gluon field of the nucleus and construct the two-dimensional color charge density for McLerran-Venugopalan model out of it. We prove that the density of states distribution, as a function of color charge density, is Gaussian, confirming the assumption made by McLerran and Venugopalan.

Paper Structure

This paper contains 5 sections, 63 equations, 1 figure.

Figures (1)

  • Figure 1: Nucleus with "nucleons" being quark-antiquark pairs.