Schroedinger and Hamilton-Jacobi equations

dc.creatorLokajicek, Milos V.
dc.date2006-11-16
dc.date.accessioned2026-07-07T07:34:13Z
dc.date.available2026-07-07T07:34:13Z
dc.descriptionTime-dependent Schroedinger equation represents the basis of any quantum-theoretical approach. The question concerning its proper content in comparison to the classical physics has not been, however, fully answered until now. It will be shown that there is one-to-one physical correspondence between basic solutions (represented always by one Hamiltonian eigenfunction only) and classical ones, as the non-zero quantum potential has not any physical sense, representing only the "numerical" difference between Hamilton principal function and the phase of corresponding wave function in the case of non-inertial motion. Possible interpretation of superposition solutions will be then discussed in the light of this fact. And also different interpretation alternatives of the quantum-mechanical model will be newly analyzed and new attitude to them will be reasoned.
dc.description7 pages
dc.identifierhttps://arxiv.org/abs/quant-ph/0611176
dc.identifierhttp://arxiv.org/abs/quant-ph/0611176
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/119735
dc.subjectQuantum Physics
dc.titleSchroedinger and Hamilton-Jacobi equations
dc.typetext

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