Speaker
Description
One of the outstanding challenges in the theory of strong interactions described by Quantum Chromodynamics is to understand its non-perturbative properties which can explain many important phenomena e.g., color confinement. In this work we study the non-perturbative sector of magnetic gluons whose momenta are given by
in a finite temperature (
excitations of the QCD plasma from the perturbative estimates at high temperatures and provide an explanation for the significant difference between these screening masses that cannot be explained within perturbative QCD.