{ "id": "hep-ph/9402213", "version": "v1", "published": "1994-02-02T23:25:45.000Z", "updated": "1994-02-02T23:25:45.000Z", "title": "Effect of Wavefunction Renormalisation in N-Flavour Qed3 at Finite Temperature", "authors": [ "I. J. R. Aitchison", "M. Klein-Kreisler" ], "comment": "17 pages + 13 figures (available upon request), Oxford preprint OUTP-93-30P, IFUNAM preprint FT94-39, LaTex", "journal": "Phys.Rev. D50 (1994) 1068-1076", "doi": "10.1103/PhysRevD.50.1068", "categories": [ "hep-ph", "cond-mat", "hep-lat", "hep-th" ], "abstract": "A recent study of dynamical chiral symmetry breaking in N-flavour QED$_3$ at finite temperature is extended to include the effect of fermion wavefunction renormalisation in the Schwinger-Dyson equations. The simple ``zero-frequency'' truncation previously used is found to lead to unphysical results, especially as $T \\to 0$. A modified set of equations is proposed, whose solutions behave in a way which is qualitatively similar to the $T=0$ solutions of Pennington et al. [5-8] who have made extensive studies of the effect of wavefunction renormalisation 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 $T \\not= 0$, and an $N-T$ phase diagram very similar to the earlier study neglecting wavefunction renormalisation. The reason for the difference is traced to the different infrared behaviour of the vacuum polarisation at $T=0$ and at $T \\not= 0$.", "revisions": [ { "version": "v1", "updated": "1994-02-02T23:25:45.000Z" } ], "analyses": { "keywords": [ "finite temperature", "n-flavour qed3", "earlier study neglecting wavefunction renormalisation", "fermion wavefunction renormalisation", "vacuum polarisation" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. D" }, "note": { "typesetting": "LaTeX", "pages": 17, "language": "en", "license": "arXiv", "status": "editable", "inspire": 371589 } } }