2009/07/13 by P. Aurenche, B. G. Zakharov, Б. Г. Захаров · 29 citations
Physics and Astronomy · #Bottom quark #Down quark #Gluon #High-Energy Particle Collisions Research #Nuclear physics #Particle physics #Particle physics theoretical and experimental studies #Photon #Physics #Plasma #Quantum Chromodynamics and Particle Interactions #Quantum electrodynamics #Quantum mechanics #Quark #Quark–gluon plasma #Radiative transfer #Top quark #Up quark #hep-ph
paper · pdf · doi:10.1134/s0021364009160048
published in Journal of Experimental and Theoretical Physics Letters 90(4), 237-243 (Pleiades Publishing) · 8 pages, 3 figures
arxiv created 2009/07/13 · openalex publication_date 2009/10/01 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We demonstrate that for a finite-size quark-gluon plasma the induced gluon radiation from heavy quarks is stronger than that for light quarks when the gluon formation length becomes comparable with (or exceeds) the size of the plasma. The effect is due to oscillations of the light-cone wave function for the in-medium q → gq transition. The dead cone model by Dokshitzer and Kharzeev neglecting quantum finite-size effects is not valid in this regime. The finite-size effects also enhance the photon emission from heavy quarks.