2017
DOI: 10.1007/s10714-017-2323-7
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Transformations of asymptotically AdS hyperbolic initial data and associated geometric inequalities

Abstract: Abstract. We construct transformations which take asymptotically AdS hyperbolic initial data into asymptotically flat initial data, and which preserve relevant physical quantities. This is used to derive geometric inequalities in the asymptotically AdS hyperbolic setting from counterparts in the asymptotically flat realm, whenever a geometrically motivated system of elliptic equations admits a solution. The inequalities treated here relate mass, angular momentum, charge, and horizon area.

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Cited by 4 publications
(7 citation statements)
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“…We would like to point the reader to the interesting work by Carrasco and Mars [10] giving insights into the (over-)generality of H = 0 as a condition for a horizon. In a recent paper of Cha and Khuri [12], the area A of the outermost STCMC-surface with H = 2 appears in the conjectured Penrose Inequality m ≥ √ A /16π expected to hold for an asymptotically anti-de Sitter initial data set of mass m satisfying the dominant energy condition. Because of the spacetime geometry nature of the STCMC-condition, we expect that STCMC-surfaces and STCMC-foliations will have a number of applications beyond the definition of a center of mass of an isolated system as well as beyond the setting of asymptotically Euclidean initial data sets.…”
Section: Introduction and Goalsmentioning
confidence: 99%
“…We would like to point the reader to the interesting work by Carrasco and Mars [10] giving insights into the (over-)generality of H = 0 as a condition for a horizon. In a recent paper of Cha and Khuri [12], the area A of the outermost STCMC-surface with H = 2 appears in the conjectured Penrose Inequality m ≥ √ A /16π expected to hold for an asymptotically anti-de Sitter initial data set of mass m satisfying the dominant energy condition. Because of the spacetime geometry nature of the STCMC-condition, we expect that STCMC-surfaces and STCMC-foliations will have a number of applications beyond the definition of a center of mass of an isolated system as well as beyond the setting of asymptotically Euclidean initial data sets.…”
Section: Introduction and Goalsmentioning
confidence: 99%
“…Her method derives from a deformation argument of Schoen and Yau [70], which involves solving the Jang equation so that the solution admits hyperboloidal asymptotics. The induced metric on the Jang graph is then asymptotically flat, with ADM mass that agrees (up to a positive multiplicative factor) with the hyperbolic mass; further generalizations of this deformation procedure have been studied in [20,19]. The desired result then follows from the positive mass theorem in the asymptotically flat setting.…”
Section: Introductionmentioning
confidence: 92%
“…Next, notice that a consequence of (8. 19) is that ∇E is symmetric, and hence E is closed as a 1-form. Since the first cohomology H 1 (M ) is trivial, there exists a globally defined function h such that E = dh.…”
Section: A Positive Mass Theorem With Chargementioning
confidence: 99%
“…This result effectively reduces the proof of the geometrical inequality to proving existence of solutions to certain equations with appropriate fall off conditions. Cha and Khuri (2017) apply the same arguments to obtain an identical global inequality to (150) in the case that the initial data has two ends, one AdS hyperbolic and the other either asymptotically AdS hyperbolic or asymptotically cylindrical. The cosmological constant is not, however, explicitly included into the inequality.…”
Section: Non Asymptotically Flat Manifoldsmentioning
confidence: 98%
“…As we discuss in Sect. 3.2, Cha and Khuri (2017) study asymptotically AdS hyperbolic initial data and prove a global inequality where the cosmological constant does not appear explicitly. They conjecture, though, that an inequality of the form…”
Section: Cosmological Constantmentioning
confidence: 99%