$\barψ ψ$-condensate in constant magnetic fields

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dc.creatorAnguiano-Galicia, M. de J.
dc.creatorBashir, A.
dc.creatorRaya, A.
dc.date2007-10-26
dc.date.accessioned2026-07-07T11:53:49Z
dc.date.available2026-07-07T11:53:49Z
dc.descriptionWe solve Dirac equation in the presence of a constant magnetic field in (3+1)- and (2+1)-dimensions. Quantizing the fermion field, we calculate $\barψ ψ$-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.
dc.description4 pages, no figures
dc.identifierhttps://arxiv.org/abs/0710.5139
dc.identifierhttp://arxiv.org/abs/0710.5139
dc.identifierPhys.Rev.D76:127702,2007
dc.identifierdoi:10.1103/PhysRevD.76.127702
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/204680
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectMesoscale and Nanoscale Physics
dc.title$\barψ ψ$-condensate in constant magnetic fields
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