Abstract

Photon-jet azimuthal correlations in proton-nucleus collisions are a promising tool for gaining information on the gluon distribution of the nucleus in the regime of non-linear color fields. We compute such correlations from the process $g+A\to q \bar{q} \gamma$ in the rapidity regime where both the projectile and target light-cone momentum fractions are small. By integrating over the phase space of the quark which emits the photon, subject to the restriction that the photon picks up most of the transverse momentum (to pass an isolation cut), we effectively obtain a $g+A\to q \gamma$ process. For nearly back-to-back photon-jet configurations we find that it dominates over the leading order process $q+A\to q \gamma$ by two less powers of $Q_\perp / Q_S$, where $\boldsymbol{Q}_\perp$ and $Q_S$ denote the net photon-jet pair momentum and the saturation scale of the nucleus, respectively. We determine the transverse momentum dependent gluon distributions involved in $g+A\to q \gamma$ and the scale where they are evaluated. Finally, we provide analytic expressions for $\langle\cos n\phi\rangle$ moments, where $\phi$ is the angle between $\boldsymbol{Q}_\perp$ and the average photon-jet transverse momentum $\tilde{\boldsymbol{P}}_\perp$, and first qualitative estimates of their transverse momentum dependence.

Highlights

  • Angular correlations between hadrons and prompt photons in high-energy collisions have been suggested to provide insight into the gluon fields of hadrons or nuclei in the small-x, nonlinear regime [1,2,3,4,5,6]

  • We show that in the back-to-back correlation limit where the photonjet transverse momentum imbalance Q⊥ 1⁄4 p⊥ þ kγ⊥ is much smaller than their average transverse momentum P~ ⊥ 1⁄4 ðp⊥ − kγ⊥Þ=2, and smaller than the saturation scale QS of the nucleus, the g → qγ process dominates over q → qγ by two powers of Q⊥=QS

  • In this paper we have computed the photon-jet cross section corresponding to the process g → qγ in the small-x regime of p þ A collisions

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Summary

INTRODUCTION

Angular correlations between hadrons and prompt photons in high-energy collisions have been suggested to provide insight into the gluon fields of hadrons or nuclei in the small-x, nonlinear regime [1,2,3,4,5,6]. References [13,14] considered photon-jet production in collinear factorization at NLO supplemented by a parton shower generator Such angular correlations from qq → γg annihilation in ppcollisions have been discussed in Ref. Photon-jet correlations in p þ p collisions have provided information on transversemomentum-dependent gluon distributions albeit not in the weakly coupled, nonlinear regime of QCD since the saturation momentum of a proton at RHIC energies (on average over impact parameters) is well below 1 GeV [18].

LEADING-ORDER PHOTON-JET CROSS SECTION
NEXT-TO-LEADING-ORDER PHOTON-JET AMPLITUDE
NEXT-TO-LEADING-ORDER CROSS SECTION
JET-PHOTON CORRELATIONS IN THE COLLINEAR APPROXIMATION
Integration over the photon-quark collinear singularity
Cross section in the correlation limit
Angular correlations
SUMMARY AND DISCUSSION
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