Wave mechanics without gauge fixing

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dc.creatorStewart, A. M.
dc.date2005-05-11
dc.date.accessioned2026-07-07T06:12:45Z
dc.date.available2026-07-07T06:12:45Z
dc.descriptionBy using the multipolar gauge it is shown that the quantum mechanics of an electrically charged particle moving in a prescribed classical electromagnetic field (wave mechanics) may be expressed in a manner that is gauge invariant, except that the only gauge functions that are allowable in a gauge transformation are those that consist of the sum of a function that depends only on the space coordinates and a term that is the product of a constant and the time coordinate. The multipolar gauge specifies the specific set of potentials that are best suited for use in the Schroedinger equation.
dc.description13 pages
dc.identifierhttps://arxiv.org/abs/quant-ph/0505079
dc.identifierhttp://arxiv.org/abs/quant-ph/0505079
dc.identifierJournal of Molecular Structure (Theochem) 626 (2003) 47-51
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/92884
dc.subjectQuantum Physics
dc.titleWave mechanics without gauge fixing
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