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Cos(4 phi) azimuthal anisotropy in small-x DIS dijet production beyond the leading power TMD limit

Adrian Dumitru, Vladimir Skokov

TL;DR

The paper addresses azimuthal anisotropies in small-x DIS dijet production beyond the leading TMD limit. It develops a fourth-order expansion of the quadrupole operator, identifies the cos 4phi azimuthal harmonic, and derives Phi2 as the key operator-valued quantity, with analytic results in a Gaussian large-Nc (MV) model. The results show cos 4phi is suppressed by 1/P^2 relative to cos 2phi but can be potentially observed at future EIC, and provide a framework for including small-x evolution in Phi2. Together, they extend the understanding of angular correlations in high-energy QCD and quantify beyond-leading-power corrections to TMD-based predictions.

Abstract

We determine the first correction to the quadrupole operator in high-energy QCD beyond the TMD limit of Weizsaecker-Williams and linearly polarized gluon distributions. These functions give rise to isotropic resp. ~ cos 2 phi angular distributions in DIS dijet production. On the other hand, the correction produces a ~ cos 4 phi angular dependence which is suppressed by one additional power of the dijet transverse momentum scale (squared) P^2.

Cos(4 phi) azimuthal anisotropy in small-x DIS dijet production beyond the leading power TMD limit

TL;DR

The paper addresses azimuthal anisotropies in small-x DIS dijet production beyond the leading TMD limit. It develops a fourth-order expansion of the quadrupole operator, identifies the cos 4phi azimuthal harmonic, and derives Phi2 as the key operator-valued quantity, with analytic results in a Gaussian large-Nc (MV) model. The results show cos 4phi is suppressed by 1/P^2 relative to cos 2phi but can be potentially observed at future EIC, and provide a framework for including small-x evolution in Phi2. Together, they extend the understanding of angular correlations in high-energy QCD and quantify beyond-leading-power corrections to TMD-based predictions.

Abstract

We determine the first correction to the quadrupole operator in high-energy QCD beyond the TMD limit of Weizsaecker-Williams and linearly polarized gluon distributions. These functions give rise to isotropic resp. ~ cos 2 phi angular distributions in DIS dijet production. On the other hand, the correction produces a ~ cos 4 phi angular dependence which is suppressed by one additional power of the dijet transverse momentum scale (squared) P^2.

Paper Structure

This paper contains 7 sections, 45 equations, 2 figures.

Figures (2)

  • Figure 1: The functions $xG^{(1)}(q^2)$, $xh^{(1)}(q^2)$ and $\Phi_2(q^2)$ in the MV model. These functions determine the amplitudes of the $\cos 2n\phi$ contributions to the dijet angular distributions for $n=0$, 1, 2, respectively. See text for details.
  • Figure 2: $\left< \cos 2\phi\right>$ and $\left< \cos 4\phi\right>$ in $\gamma_L^*+A\to q+\bar{q}$ dijet production from the MV model. See text for details.