$\bar{\psi} \psi$-condensate in constant magnetic fields
High Energy Physics - Phenomenology
2008-11-26 v1 Mesoscale and Nanoscale Physics
Abstract
We solve Dirac equation in the presence of a constant magnetic field in (3+1)- and (2+1)-dimensions. Quantizing the fermion field, we calculate -condensate from first principles for parity conserving and violating Lagrangians for arbitrary field strength. We make comparison with the results already known in the literature for some particular cases and point out the relevance of our work for possible physical applications.
Cite
@article{arxiv.0710.5139,
title = {$\bar{\psi} \psi$-condensate in constant magnetic fields},
author = {M. de J. Anguiano-Galicia and A. Bashir and A. Raya},
journal= {arXiv preprint arXiv:0710.5139},
year = {2008}
}
Comments
4 pages, no figures