Geometric phase and chiral anomaly; their basic differences

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dc.creatorFujikawa, Kazuo
dc.date2008-02-28
dc.date.accessioned2026-07-07T12:39:41Z
dc.date.available2026-07-07T12:39:41Z
dc.descriptionAll the geometric phases are shown to be topologically trivial by using the second quantized formulation. The exact hidden local symmetry in the Schrödinger equation, which was hitherto unrecognized, controls the holonomy associated with both of the adiabatic and non-adiabatic geometric phases. The second quantized formulation is located in between the first quantized formulation and the field theory, and thus it is convenient to compare the geometric phase with the chiral anomaly in field theory. It is shown that these two notions are completely different.
dc.description15 pages
dc.identifierhttps://arxiv.org/abs/0802.4157
dc.identifierhttp://arxiv.org/abs/0802.4157
dc.identifierInt.J.Mod.Phys.A23:4933-4944,2008
dc.identifierdoi:10.1142/S0217751X08042833
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/219196
dc.subjectHigh Energy Physics - Theory
dc.titleGeometric phase and chiral anomaly; their basic differences
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