2003/07/31 by Jamal Jalilian-Marian, Yasushi Nara, Raju Venugopalan · 5 citations
Physics and Astronomy · #Color-glass condensate #Geometry #Gluon #Heavy ion #High-Energy Particle Collisions Research #Ion #Nuclear physics #Particle physics theoretical and experimental studies #Physics #Quantum #Quantum Chromodynamics and Particle Interactions #Quantum electrodynamics #Quantum mechanics #Quark #Scaling #Twist #hep-ph #nucl-ex #nucl-th
paper · pdf · doi:10.1016/j.physletb.2003.09.097
published as Phys.Lett.B577:54-60,2003 · 6pages, 4figures, revised version
openalex publication_date 2003/11/01 · arxiv created 2003/11/05 · arxiv updated 2010/11/30 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We show that the numerical solution of the classical SU(3) Yang-Mills equations of motion in the McLerran-Venugopalan model for gluon production in central heavy ion collisions leads to a suppresion at low pt and an enhancement at the intermediate pt region as compared to peripheral heavy ion and pp collisions at the same energy. Our results are compared to previous, Color Glass Condensate inspired calculations of gluon production in heavy ion collisions. We revisit the predictions of the Color Glass Condensate model for pA (dA) collisions in Leading Order and show that quantum evolution--in particular the phenomenon of geometric scaling and change of anomalous dimensions--preserves the Cronin enhancement of pA cross section (when normalized to the leading twist term) in the Leading Order approximation even though the pt spectrum can change. We comment on the case when gluon radiation is included.