Abstract

We show that the cross section for diffractive dissociation of a small onium off a large nucleus at total rapidity $Y$ and requiring a minimum rapidity gap ${Y}_{\mathrm{gap}}$ can be identified, in a well-defined parametric limit, with a simple classical observable on the stochastic process representing the evolution of the state of the onium, as its rapidity increases, in the form of color dipole branchings: it formally coincides with twice the probability that an even number of these dipoles effectively participate in the scattering, when viewed in a frame in which the onium is evolved to the rapidity $Y\ensuremath{-}{Y}_{\mathrm{gap}}$. Consequently, finding asymptotic solutions to the Kovchegov-Levin equation, which rules the $Y$ dependence of the diffractive cross section, boils down to solving a probabilistic problem. Such a formulation authorizes the derivation of a parameter-free analytical expression for the gap distribution. Interestingly enough, events in which many dipoles interact simultaneously play an important role, since the distribution of the number $k$ of dipoles participating in the interaction turns out to be proportional to $1/[k(k\ensuremath{-}1)]$.

Highlights

  • In an appropriate frame, the electron-hadron interaction is mediated by a colorless quarkantiquark fluctuation of a virtual photon picked in the state of the electron [9,10]

  • Diffractive events are traditionally split into two classes: quasielastic scattering events, in which the diffractive system typically consists in a vector meson or in a hadronized open quark-antiquark pair, and high-mass diffractive dissociation events, in which the diffractive system possesses an invariant mass on the order of the center-of-mass energy of the onium-hadron subreaction, and a sizable multiplicity

  • While the former have drawn a lot of attention recently, less effort has been devoted to the latter

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Summary

Introduction

Diffraction has been observed in the scattering of protons and nuclei [1,2]; more unexpectedly, in deep-inelastic electron-proton scattering [3–5]. Diffractive events are traditionally split into two classes: quasielastic scattering events, in which the diffractive system typically consists in a vector meson or in a hadronized open quark-antiquark pair, and high-mass diffractive dissociation events, in which the diffractive system possesses an invariant mass on the order of the center-of-mass energy of the onium-hadron subreaction, and a sizable multiplicity. While the former have drawn a lot of attention recently

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