Localised Dirac eigenmodes, chiral symmetry breaking, and Goldstone's theorem at finite temperature
arXiv:2009.00486 · doi:10.1088/1751-8121/ac1c3a
Abstract
I show that a finite density of near-zero localised Dirac modes in the chirally broken phase of a gauge theory can lead to the disappearance of the massless excitations predicted by the Goldstone theorem at finite temperature.
Revised version: title changed; error corrected in Eq. 11, conclusions unchanged; discussion improved, comments added about symmetry breaking and relation with Goldstone's theorem; published version, 13 pages
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Cited by in corpus (6)
- Eigenvalue spectra of QCD and the fate of breaking towards the chiral limit
- Localization of Dirac Fermions in Finite-Temperature Gauge Theory
- Localization of Dirac modes in finite-temperature gauge theory on the lattice
- 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
- Localisation of Dirac eigenmodes and confinement in gauge theories: the Roberge-Weiss transition