2006/12/19 by N. O. Agasian, Yu. A. Simonov, Agasian, N. O. +1
Physics and Astronomy · #FOS: Physical sciences #High Energy Physics - Lattice (hep-lat) #High Energy Physics - Phenomenology (hep-ph) #High Energy Physics - Theory (hep-th) #High-Energy Particle Collisions Research #Nuclear Theory (nucl-th) #Quantum, superfluid, helium dynamics #Theoretical and Computational Physics #hep-lat #hep-ph #hep-th #nucl-th
paper · pdf · doi:10.48550/arxiv.hep-ph/0612233
4 pages, 1 figure. Talk given at the XXXIII International Conference on High Energy Physics (ICHEP06), Moscow, Russia, 26 July - 02 August 2006;v2: minor misprints corrected; few references added
openalex publication_date 2006/12/19 · arxiv created 2007/07/09 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
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 and σs=σs(T) is the spatial string tension. The resulting magnitude of mD(T) and temperature dependence are in good agreement with lattice calculations.