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New nonperturbative approach to the Debye mass in hot QCD

2006/04/30 by N. O. Agasian, Yu. A. Simonov · 2 citations
Physics and Astronomy · #Chiral perturbation theory #Condensed matter physics #Debye #High-Energy Particle Collisions Research #Invariant (physics) #Lattice (music) #Lattice QCD #Lattice field theory #Mathematical physics #Particle physics #Particle physics theoretical and experimental studies #Perturbation theory (quantum mechanics) #Physics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Quantum electrodynamics #hep-lat #hep-ph #hep-th #nucl-th

paper · pdf · doi:10.1016/j.physletb.2006.06.019

published as Phys.Lett.B639:82-87,2006 · 14 pages, 4 figures; new figures and discussion added; to appear in Phys.Lett.B

arxiv created 2006/06/13 · openalex publication_date 2006/06/22 · arxiv updated 2014/11/17 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

The Debye mass mD is computed nonperturbatively in the deconfined phase of QCD, where chromomagnetic confinement is known to be present. The latter defines mD to be mD=cD√(σs), where cD ≅ 2.06 and σss(T) is the spatial string tension. The resulting magnitude of mD(T) and temperature dependence are in good agreement with lattice calculations. Background perturbation theory expansion for mD(T) is discussed in comparison to standard perturbative results and recent gauge-invariant definitions.

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