51. Proper static potential in classical lattice gauge theory at finite T
- Author
-
Alexander Rothkopf and Alexander Lehmann
- Subjects
Quark ,Nuclear and High Energy Physics ,High Energy Physics::Lattice ,FOS: Physical sciences ,Lattice QCD ,QC770-798 ,01 natural sciences ,Theoretical physics ,High Energy Physics - Phenomenology (hep-ph) ,High Energy Physics - Lattice ,Interaction potential ,Lattice gauge theory ,Nuclear and particle physics. Atomic energy. Radioactivity ,0103 physical sciences ,010306 general physics ,Quantum ,Physics ,Matematikk og Naturvitenskap: 400::Fysikk: 430 [VDP] ,Lattice Quantum Field Theory ,010308 nuclear & particles physics ,High Energy Physics - Lattice (hep-lat) ,Gauss ,High Energy Physics::Phenomenology ,Gauge (firearms) ,High Energy Physics - Phenomenology ,Quark–gluon plasma ,Quark-Gluon Plasma - Abstract
We compute the proper real-time interaction potential between a static quark and antiquark in classical lattice gauge theory at finite temperature. Our central result is the determination of the screened real-part of this potential, and we reconfirm the presence of an imaginary part. The real part is intimately related to the back-reaction of the static sources onto the gauge fields, incorporated via Gauss's law. Differences in the treatment of static sources in quantum and classical lattice gauge theory are discussed., 24 pages, 10 figures, supplementary material: 2 Mathematica scripts, source code available on Zenodo
- Published
- 2021