Localisation in 2+1 dimensional SU(3) pure gauge theory at finite temperature
arXiv:1903.04983 · doi:10.1007/JHEP05(2019)204
Abstract
I study the localisation properties of low Dirac eigenmodes in 2+1 dimensional SU(3) pure gauge theory, both in the low-temperature, confined and chirally-broken phase and in the high-temperature, deconfined and chirally-restored phase, by means of numerical lattice simulations. While these modes are delocalised at low temperature, they become localised at high temperature, up to a critical point in the Dirac spectrum where a BKT-type Anderson transition takes place. All results point to localisation appearing at the deconfinement temperature, and support previous expectations about the close relation between deconfinement, chiral symmetry breaking, and localisation.
1+33 pages, 16 figures; several minor changes (typos fixed, a few remarks and extra references added); matches published version
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Cited by in corpus (9)
- Localization of Dirac Fermions in Finite-Temperature Gauge Theory
- Reconfinement, localization and thermal monopoles in trace-deformed Yang-Mills theory
- 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
- Deconfinement transition and localization of Dirac modes in finite-temperature gauge theory on the lattice
- Localisation of Dirac modes in gauge theories and Goldstone's theorem at finite temperature
- QCD Anderson transition with overlap valence quarks on a twisted-mass sea
- Localisation of Dirac eigenmodes and confinement in gauge theories: the Roberge-Weiss transition