On the Quantization Procedure in Classical Mechanics and Problem of Hidden Variables in Bohmian Mechanics

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dc.creatorRusov, V. D.
dc.creatorVlasenko, D.
dc.date2008-06-25
dc.date2008-09-01
dc.date.accessioned2026-07-07T09:59:22Z
dc.date.available2026-07-07T09:59:22Z
dc.descriptionBasing on the Chetaev's theorem on stable trajectories in dynamics in the presence of dissipative forces we obtain a generalized stability condition for Hamiltonian systems that has the form of the Schrodinger equation. We show that the energy of the dissipative forces generating generalized Chetaev's stability condition exactly coincides with Bohm's "quantum" potential. Using the principle of least action of perturbation we prove that the Bohmian quantum mechanics complemented with the Chetaev's generalized theorem does not have hidden variables.
dc.description15 pages
dc.identifierhttps://arxiv.org/abs/0806.4050
dc.identifierhttp://arxiv.org/abs/0806.4050
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/167995
dc.subjectQuantum Physics
dc.titleOn the Quantization Procedure in Classical Mechanics and Problem of Hidden Variables in Bohmian Mechanics
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