Localised Dirac eigenmodes, chiral symmetry breaking, and Goldstone’s theorem at finite temperature. (English) Zbl 1520.81137
Summary: 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.
MSC:
| 81T28 | Thermal quantum field theory |
| 81R40 | Symmetry breaking in quantum theory |
| 81T13 | Yang-Mills and other gauge theories in quantum field theory |
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