2018
DOI: 10.1103/physrevd.97.044028
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Freud’s superpotential in general relativity and in Einstein-Cartan theory

Abstract: The identification of a suitable gravitational energy in theories of gravity has a long history, and it is well known that a unique answer cannot be given. In the first part of this paper we present a streamlined version of the derivation of Freud's superpotential in general relativity. It is found if we once integrate the gravitational field equation by parts. This allows us to extend these results directly to the Einstein-Cartan theory. Interestingly, Freud's original expression, first stated in 1939, remain… Show more

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Cited by 7 publications
(6 citation statements)
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References 34 publications
(37 reference statements)
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“…Equivalently in terms of tensors, the object with vanishing (Levi-Civita) divergence is T eff µν as defined in (22), and it provides the conserved energy-momentum tensor of the theory. 4 This simple observation is well-known in the literature, see [12,13,26] (where it is referred to as 'combined energy-momentum tensor'), and can be taken to provide the basis of energy conservation in Einstein-Cartan theory.…”
Section: Noether Identities and Conservation Lawsmentioning
confidence: 93%
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“…Equivalently in terms of tensors, the object with vanishing (Levi-Civita) divergence is T eff µν as defined in (22), and it provides the conserved energy-momentum tensor of the theory. 4 This simple observation is well-known in the literature, see [12,13,26] (where it is referred to as 'combined energy-momentum tensor'), and can be taken to provide the basis of energy conservation in Einstein-Cartan theory.…”
Section: Noether Identities and Conservation Lawsmentioning
confidence: 93%
“…There are three problems that we can see with this construction. First, a Killing vector is metricgeodesic, but in general not geodesic with respect to the torsion-full connection, since from (13) we see that…”
Section: Non-equilibrium Approachmentioning
confidence: 98%
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“…φ = −ψ. Only scalars and vectors contribute to either (153) or (154) and there is no energy due to tensor modes. We will have a closer look at the transverse-traceless components h ij , which are the only components that may propagate in vacuum.…”
Section: A Linear Perturbationsmentioning
confidence: 99%
“…Previously, Wallner and Thirring [1,2] explicitly showed that using the expression for the Thirring 2-forms, it is possible to obtain sundry energy definitions of energy, given by for example, Freud [3], Møller [4,5], and Landau and Lifschitz [6]. See also the recent paper by Böhmer and Hehl [7]. Here, we elaborate on the reformulation of the Abbott-Deser energy definition in terms of differential forms that helps to gain further insight into complicated mathematical expressions.…”
mentioning
confidence: 99%