arXiv · gr-qc/0001095
A Metric Theory of Gravity with Condensed Matter Interpretation
Abstract
We 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.
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I. Schmelzer. 2000-05-16. A Metric Theory of Gravity with Condensed Matter Interpretation. https://arxiv.org/abs/gr-qc/0001095
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