1996
DOI: 10.1103/physrevd.54.3892
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Conserved masses in GHS Einstein and string black holes and consistent thermodynamics

Abstract: We analyze the relationship between quasilocal masses calculated for solutions of conformally related theories. We show that the adm mass of a static, spherically symmetric solution is conformally invariant (up to a constant factor) only if the background action functional is conformally invariant. Thus, the requirement of conformal invariance places restrictions on the choice of reference spacetimes. We calculate the mass of the black hole solutions obtained by Garfinkle, Horowitz, and Strominger (ghs) for bo… Show more

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Cited by 51 publications
(80 citation statements)
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“…The reason was clearly stated in ref. [101,100]. Even though it is possible to make the unregularized energy conformally invariant for a selected class of models, the subtraction term will inevitably destroy that invariance since an "empty" reference space is mapped into a non-trivial configuration.…”
Section: Adm Mass and Quasilocal Energymentioning
confidence: 99%
“…The reason was clearly stated in ref. [101,100]. Even though it is possible to make the unregularized energy conformally invariant for a selected class of models, the subtraction term will inevitably destroy that invariance since an "empty" reference space is mapped into a non-trivial configuration.…”
Section: Adm Mass and Quasilocal Energymentioning
confidence: 99%
“…The background must be chosen such that its topological properties match the solution whose action and conserved charges we want to compute. However, this does not unequivocally fix the choice of the background [2] and moreover, there might be cases in which the topological properties of the solution rule out any natural choice of the background.…”
Section: Introductionmentioning
confidence: 99%
“…By using a new local, covariant counterterm they obtained conserved quantities that agree with older definitions known in literature. In particular, they constructed a boundary stress-tensor similar with the one used in quasi-local context [8,2], which in the so-called 'hyperbolic cut-off' has been shown to lead to conserved quantities that are built out of the electric part of the Weyl tensor, similar to the Ashtekar-Hansen expressions in four dimensions [10]. The connection with the Ashtekar-Hansen conserved quantities has been examined in more detail in [11], in which it was argued that the canonical form of the action built using the MannMarolf (MM) counterterm reduces to the ADM action [12].…”
Section: Introductionmentioning
confidence: 99%
“…Unfortunately it suffers from several drawbacks. The choice of reference spacetime is not always unique [12], nor is it always possible to embed a boundary with a given induced metric into the reference background. Indeed, for Kerr spacetimes, this latter problem forms a serious obstruction towards calculating the subtraction energy, and calculations have only been performed in the slow-rotating regime [13].…”
Section: Introductionmentioning
confidence: 99%