QCD Perspectives on Hot and Dense Matter 2002
DOI: 10.1007/978-94-010-0267-7_5
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Regge Poles in QCD and Heavy-Ion Collisions

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“…This reduction is dependent on the nuclear mass, and has been successfully understood within the Vector Meson Dominance model (VMD), which describes the photon's wave function as a superposition of mesonic states (ρ, ω, ϕ) [48,49,59] that interact hadronically with the nucleus. At higher energies, where the photon can resolve the partons in the nucleus, the parton distribution function is predicted to be high enough that the nucleus becomes opaque to photons, leading to a theoretical limit similar to that of hadron-nucleus interactions α lim = 2/3 [50]. The mass scaling is typically parametrized in the literature as a power of the nuclear mass:…”
Section: Jcap11(2019)007mentioning
confidence: 99%
“…This reduction is dependent on the nuclear mass, and has been successfully understood within the Vector Meson Dominance model (VMD), which describes the photon's wave function as a superposition of mesonic states (ρ, ω, ϕ) [48,49,59] that interact hadronically with the nucleus. At higher energies, where the photon can resolve the partons in the nucleus, the parton distribution function is predicted to be high enough that the nucleus becomes opaque to photons, leading to a theoretical limit similar to that of hadron-nucleus interactions α lim = 2/3 [50]. The mass scaling is typically parametrized in the literature as a power of the nuclear mass:…”
Section: Jcap11(2019)007mentioning
confidence: 99%