Localisation of Dirac eigenmodes and confinement in gauge theories: the Roberge-Weiss transition
arXiv:2211.11507 · doi:10.1051/epjconf/202227402009
Abstract
Ample numerical evidence from lattice calculations shows a strong connection between the confining properties of gauge theories at finite temperature and the localisation properties of the low-lying Dirac eigenmodes. In this contribution we discuss recent progress on this topic, focussing on results for QCD at imaginary chemical potential at temperatures above the Roberge-Weiss transition temperature. These confirm the general picture of low modes turning from delocalised to localised at the deconfinement transition, in a previously unexplored setup with a genuine, physical transition in the presence of dynamical fermions. This further supports the use of Dirac eigenmodes as a tool to investigate the mechanisms behind confinement and the deconfinement transition.
8 pages, 4 figures; contribution to the proceedings of the XVth Quark Confinement and Hadron Spectrum conference (ConfXV), 1-6 August 2022, University of Stavanger, Stavanger (Norway)
References in corpus (11)
- Anderson Transitions
- Chiral phase transition in lattice QCD as a metal-insulator transition
- Anderson Localization in Quark-Gluon Plasma
- An Ising-Anderson model of localisation in high-temperature QCD
- Localization of Dirac Fermions in Finite-Temperature Gauge Theory
- Deconfinement, chiral transition and localisation in a QCD-like model
- Reconfinement, localization and thermal monopoles in trace-deformed Yang-Mills theory
- Localisation in 2+1 dimensional SU(3) pure gauge theory at finite temperature
- Localization of Dirac modes in finite-temperature gauge theory on the lattice
- Localization properties of Dirac modes at the Roberge-Weiss phase transition
- Localised Dirac eigenmodes, chiral symmetry breaking, and Goldstone's theorem at finite temperature