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Wilson line correlator in the MV model: relating the glasma to deep inelastic scattering

2007/11/30 by T. Lappi · 6 citations
Mathematics · Physics and Astronomy · #Color-glass condensate #Computation #Deep inelastic scattering #Discretization #Gluon #Hadron #High-Energy Particle Collisions Research #Inelastic collision #Inelastic scattering #Mathematical analysis #Mathematics #Multiplicity (mathematics) #Nuclear physics #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Quantum electrodynamics #Quantum mechanics #Scattering #hep-ph #nucl-th

paper · pdf · doi:10.1140/epjc/s10052-008-0588-4

published as Eur.Phys.J.C55:285-292,2008 · 8 pages, 10 figures, RevTEX4, V2: typo corrections, V3: small clarifications, to be published in EPJ C

arxiv created 2008/03/21 · openalex publication_date 2008/04/23 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

In the color glass condensate framework the saturation scale measured in deep inelastic scattering of high energy hadrons and nuclei can be determined from the correlator of Wilson lines in the hadron wavefunction. These same Wilson lines give the initial condition of the classical field computation of the initial gluon multiplicity and energy density in a heavy ion collision. In this paper the Wilson line correlator in both adjoint and fundamental representations is computed using exactly the same numerical procedure that has been used to calculate gluon production in a heavy ion collision. In particular the discretization of the longitudinal coordinate has a large numerical effect on the relation between the color charge density parameter g2 mu and the saturation scale Qs. Our result for this relation is Qs = 0.6 g2 mu, which results in the classical Yang-Mills value for the "gluon liberation coefficient" c = 1.1.

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