A Metric Theory of Gravity with Condensed Matter Interpretation

dc.creatorSchmelzer, I.
dc.date2000-01-28
dc.date2000-05-16
dc.date.accessioned2026-07-07T03:24:44Z
dc.date.available2026-07-07T03:24:44Z
dc.descriptionWe consider a classical condensed matter theory in a Newtonian framework where conservation laws \partial_t ρ+ \partial_i (ρv^i) = 0 \partial_t (ρv^j) + \partial_i(ρv^i v^j + p^{ij}) = 0 are related with the Lagrange formalism in a natural way. For an ``effective Lorentz metric'' g_{μν} it is equivalent to a metric theory of gravity close to general relativity with Lagrangian L = L_{GR} - (8πG)^{-1}(Υg^{00}-Ξ(g^{11}+g^{22}+g^{33}))\sqrt{-g} We consider the differences between this theory and general relativity (no nontrivial topologies, stable frozen stars instead of black holes, big bounce instead of big bang singularity, a dark matter term), quantum gravity, and the connection with realism and Bohmian mechanics.
dc.description16 pages Latex, no figures. Short version of gr-qc/0001101. (The "original" version was a duplicate of gr-qc/0001101 created by a mistake.)
dc.identifierhttps://arxiv.org/abs/gr-qc/0001095
dc.identifierhttp://arxiv.org/abs/gr-qc/0001095
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/33445
dc.subjectGeneral Relativity and Quantum Cosmology
dc.titleA Metric Theory of Gravity with Condensed Matter Interpretation
dc.typetext

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