Abstract
We construct the gauge invariant fermion correlator in the Schwinger model on the torus. At zero temperature, this correlator falls off with a rate given by the Coulomb energy of an infinitely heavy charge. At high temperature, the screening mass approaches πT/2, and this in the presence of a mass gap. The fractional Matsubara frequency arises from the action of a pair of induced merons at high temperature that are localized over a range on the order of the meson Compton wavelength 1/m=. We discuss the quenched approximation in this model, and comment on the possible relevance of some of these results to higher dimensions.
| Original language | English |
|---|---|
| Pages (from-to) | 5915-5923 |
| Number of pages | 9 |
| Journal | Physical Review D |
| Volume | 51 |
| Issue number | 10 |
| DOIs | |
| State | Published - 1995 |
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