Equivalence of matter-type modified gravity theories to general relativity with nonminimal matter interaction

Abstract

We show that gravity models, such as f(Lm)f(\mathcal{L}_{\rm m}), f(gμνTμν)f(g_{\mu\nu} T^{\mu\nu}) and f(TμνTμν)f(T_{\mu\nu} T^{\mu\nu}), that modify the introduction of the material source in the usual Einstein-Hilbert action by adding only matter-related terms to the matter Lagrangian density Lm\mathcal{L}_{\rm m} are equivalent to general relativity with nonminimal interactions. Through the redefinition Lm+fLmtot\mathcal{L}_{\rm m}+f \rightarrow \mathcal{L}_{\rm m}^{\rm tot}, these models are exactly GR, yet the usual material field TμνT_{\mu\nu} and its accompanying partner, viz., the modification field TμνmodT_{\mu\nu}^{\rm mod} interact nonminimally. That is, μTμν=Qν=μTμνmod\nabla^{\mu}T_{\mu\nu}=-Q_{\nu}=-\nabla^{\mu}T_{\mu\nu}^{\rm mod}, where QνQ_{\nu} is the interaction kernel that governs the rate of energy transfer. We focus on the particular model, the energy-momentum squared gravity, where the usual material field TμνT_{\mu\nu} brings in an accompanying energy-momentum squared field , TμνemsfT_{\mu\nu}^{\rm emsf} along with a sui generis nonminimal interaction between them. Compared to usual phenomenological nonminimal interaction models in the literature, EMSF gives rise to more intricate interaction kernels having covariant formulation even with simple forms of the ff function. We elaborate upon EMSF via some different aspects: a DE component induced from the interaction of sources such as cold dark matter and relativistic species with their accompanying EMSFs generating interacting DE-DM models, mimicking noncanonical scalar field, etc., or a Hoyle-type creation field generating steady-state universe models extended to fluids other than dust and a mimicker of modified generalized Chaplygin gas. We also demonstrate the proper calculation of second metric variation of Lm\mathcal{L}_{\rm m}, as well as in models that contain scalars like gμνTμν,RμνTμνg_{\mu\nu} T^{\mu\nu}\,,R_{\mu\nu}T^{\mu\nu} and GμνTμνG_{\mu\nu} T^{\mu\nu}.Comment: 16 pages, no figures and table

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