EFFECT OF WAVE-FUNCTION RENORMALIZATION IN N-FLAVOR 3-DIMENSIONAL QED AT FINITE-TEMPERATURE

A recent study of dynamical chiral symmetry breaking in N flavor three-dimensional QED at finite temperature is extended to include the effect of fermion wave function renormalization in the Schwinger-Dyson equations. The simple ''zero-frequency'' truncation previously used is found to lead to unphysical results, especially as T --> 0. A modified set of equations is proposed, whose solutions behave in a way which is qualitatively similar to the T = 0 solutions of Pennington and co-workers who have made extensive studies of the effect of wave function renormalization in this context, and who concluded that there was no critical N(c) (at T = 0) above which chiral symmetry was restored. In contrast, we find that our modified equations predict a critical N(c) at T not-equal 0, and an N-T phase diagram very similar to the earlier study neglecting wave function renormalization. The reason for the difference is traced to the different infrared behavior of the vacuum polarization at T = 0 and at T not-equal 0.