2005
DOI: 10.1016/j.nuclphysa.2005.08.025
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On the projectile-target duality of the color glass condensate in the dipole picture

Abstract: Recently Kovner and Lublinsky proposed a set of equations which can be viewed as dual to JIMWLK evolution. We show that these dual equations have a natural dipole-like structure, as conjectured by Kovner and Lublinsky. In the high energy large N c limit these evolution equations reduce to equations previously derived in the dipole model. We also show that the dual evolution kernel is scheme dependent, although its action on the weight functional describing a high energy state gives a unique result.

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Cited by 27 publications
(32 citation statements)
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“…This amounts to a different reorganization of the perturbation theory in the weak-scattering regime, which however leads to the same high-energy behaviour, as previously argued in Refs. [52,53]. (The subsequent discussion is in fact adapted For more clarity, assume that the target starts at Y = 0 as a single particle located at x 0 .…”
Section: A On the Fluctuation Terms In The Pomeron Loop Equationsmentioning
confidence: 99%
“…This amounts to a different reorganization of the perturbation theory in the weak-scattering regime, which however leads to the same high-energy behaviour, as previously argued in Refs. [52,53]. (The subsequent discussion is in fact adapted For more clarity, assume that the target starts at Y = 0 as a single particle located at x 0 .…”
Section: A On the Fluctuation Terms In The Pomeron Loop Equationsmentioning
confidence: 99%
“…The latest developments in this dynamic field are related to what is sometimes called Pomeron loops, or Fluctuations or alternatively Saturation effects in the projectile wave function [13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35]. The corrections due to these effects clearly must be important for the preasymptotic regime, but should also affect the more exclusive observables at very high energy.…”
Section: Introductionmentioning
confidence: 99%
“…Much has been understood during the last year, but many questions remain open. In particular the structure of the "Hilbert space" on which the evolution kernel acts [24] as well as the precise physical meaning of the Dense-Dilute Duality (DDD) introduced in [26] are being actively debated [28,31,32,33,34]. This paper presents several remarks on these issues.…”
Section: Introductionmentioning
confidence: 99%
“…The target distribution is then obtained by successively acting with the creation operators on the 'dipole vacuum', and can be represented as the following 'color glass weight function' : 18) where the functional distribution δ[ρ] represents the vacuum (no color charge, and hence no dipole ! ),…”
Section: A Dipolar Picture and Its Limitationsmentioning
confidence: 99%