Theory of thin shells in general relativity: Equivalence of direct and Wheeler-DeWitt quantizations

dc.creatorZloshchastiev, Konstantin G.
dc.date1997-09-12
dc.date1998-09-22
dc.date.accessioned2026-07-07T09:03:05Z
dc.date.available2026-07-07T09:03:05Z
dc.descriptionWe justify the way of the direct quantization which means immediate quantization of a conservation law. It is shown that this approach is equivalent to introducing the super Hamiltonian on a minisuperspace in spirit of the Wheeler-DeWitt's approach. Then we will have: (i) all values are observable and have an obvious physical meaning and well-defined application domain; (ii) wave function is well-defined without time slicing and often can be exactly obtained; (iii) we can take off major mathematical troubles, and therefore, more complicate models can be considered exactly without the perturbation theory.
dc.description5 pages, LaTeX
dc.identifierhttps://arxiv.org/abs/gr-qc/9709030
dc.identifierhttp://arxiv.org/abs/gr-qc/9709030
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/148874
dc.subjectGeneral Relativity and Quantum Cosmology
dc.titleTheory of thin shells in general relativity: Equivalence of direct and Wheeler-DeWitt quantizations
dc.typetext

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