Abstract

The Pomeron Regge trajectory underlies the dynamics dependence of hadronic total cross sections and diffractive reactions at high energies. The physics of the Pomeron is closely related to the gluon distribution function and the gluon gravitational form factor of the target hadron. In this article we examine the scale dependence of the nonperturbative gluon distribution in the nucleon and the pion, which was derived in a previous article [G. F. de T\'eramond, H. G. Dosch, T. Liu, R. S. Sufian, S. J. Brodsky, and A. Deur, Gluon matter distribution in the proton and pion from extended holographic light-front QCD, Phys. Rev. D 104, 114005 (2021)] in the framework of holographic light-front QCD and the Veneziano model. We argue that the QCD evolution of the gluon distribution function $g(x,\ensuremath{\mu})$ to large ${\ensuremath{\mu}}^{2}$ leads to a single scale-dependent Pomeron. The resulting Pomeron trajectory ${\ensuremath{\alpha}}_{P}(t,\ensuremath{\mu})$ not only depends on the momentum transfer squared $t$, but also on the physical scale $\ensuremath{\mu}$ of the amplitude, such as the virtuality ${Q}^{2}$ of the interacting photon in inclusive diffractive electroproduction, thus unifying the soft and the perturbative Pomeron. This can explain not only the ${Q}^{2}$ evolution of the proton structure function ${F}_{2}(x,{Q}^{2})$ at small $x$, but also the observed energy and ${Q}^{2}$ dependence of high energy diffractive processes involving virtual photons up to LHC energies.

Highlights

  • Despite the successful applications of perturbative quantum chromodynamics in describing hadronic physics at short distances, many complexities in the soft domain characterizing small momentum-transfer scattering processes at high energies remain unsolved

  • We have studied the scale dependence μ of the Pomeron trajectory intercept αð0; μÞ, which controls small-x diffractive processes

  • We have related the Pomeron intercept to the scale evolution of the intrinsic gluon distribution function obtained in Ref. [1] in the framework of holographic light-front QCD, together with the constraints imposed by the generalized Veneziano model

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Summary

INTRODUCTION

Despite the successful applications of perturbative quantum chromodynamics (pQCD) in describing hadronic physics at short distances, many complexities in the soft domain characterizing small momentum-transfer scattering processes at high energies remain unsolved. By using the warped-space gauge/gravity framework for large-NC QCD-like theories, Brower, Polchinski, Strassler, and Tan derived a simultaneous description of both the BFKL hard regime and the classic Regge soft domain [36]. Their model is consistent with some salient general features, which one would expect from the hard BFKL Pomeron at negative values of the momentum transfer t and with a glueball spectrum at positive t. It provides a natural way to compute intrinsic nonperturbative quantities at the hadronic scale, which can be evolved to higher scales using the renormalization group equations (RGE) of pQCD In this approach, the Pomeron intercept determines the small-x behavior of the gluon distribution function of a hadron.

THE POMERON INTERCEPT AND THE GLUON DISTRIBUTION IN THE HADRON
SCALE DEPENDENCE OF DIFFRACTIVE PROCESSES
A SINGLE POMERON
SUMMARY AND CONCLUSION
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