Abstract:We formulate and prove the Lorentzian version of the positive mass theorems with arbitrary negative cosmological constant for asymptotically AdS spacetimes. This work is the continuation of the second author's recent work on the positive mass theorem on asymptotically hyperbolic 3-manifolds.
“…4λ 2 e j · e i · φ α + 1 4λ 2 e i · e j · φ α (14) follows from the similar argument of the second theorem in [14]. The result that M is hyperbolic and maximal becomes a consequence that there is a basis {φ α } parallel to the imaginary Killing connection.…”
Section: Proof Of the Main Theoremsmentioning
confidence: 81%
“…Thanks to the Lax-Milgram theorem [18] , by similar argument in [11,13,14,17,19,20], there exists a unique spinor Φ 1 in H 1 (S) such that…”
We provide two new positive mass theorems under respective modified energy conditions allowing T00 negative on some compact set for certain modified asymptotically hyperbolic manifolds. This work is analogous to Zhang's previous result for modified asymptotically flat initial data sets.
“…4λ 2 e j · e i · φ α + 1 4λ 2 e i · e j · φ α (14) follows from the similar argument of the second theorem in [14]. The result that M is hyperbolic and maximal becomes a consequence that there is a basis {φ α } parallel to the imaginary Killing connection.…”
Section: Proof Of the Main Theoremsmentioning
confidence: 81%
“…Thanks to the Lax-Milgram theorem [18] , by similar argument in [11,13,14,17,19,20], there exists a unique spinor Φ 1 in H 1 (S) such that…”
We provide two new positive mass theorems under respective modified energy conditions allowing T00 negative on some compact set for certain modified asymptotically hyperbolic manifolds. This work is analogous to Zhang's previous result for modified asymptotically flat initial data sets.
“…Initial investigations were carried out in [1,3,27,30], the time symmetric case (k = 0) was treated in [2,18,19,49,53], and the most general versions were given in [20,38,50,52]. See also [15] for a discussion concerning the rigidity statement.…”
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.
“…In this section, we use hyperbolic coordinates and the positive mass theorem for asymptotically hyperbolic manifolds proved in [31,28] to derive a positive mass theorem for asymptotically half de Sitter spacetime. Let…”
Section: Hyperbolic Coordinates and Positive Mass Theoremmentioning
confidence: 99%
“…Anti-de Sitter spacetimes are characterized by Killing spinors with imaginary Killing constants, which have certain nice properties. Witten's method was extended successfully to asymptotically Antide Sitter spacetimes and the positive mass theorem was proved completely and rigorously in this case [25,10,31,17,28]. As recent cosmological observations indicated that our universe possibly has a positive cosmological constant, the positive mass theorem for asymptotically de Sitter spacetimes gains much more importance.…”
Abstract. We use planar coordinates as well as hyperbolic coordinates to separate the de Sitter spacetime into two parts. These two ways of cutting the de Sitter give rise to two different spatial infinities. For spacetimes which are asymptotic to either half of the de Sitter spacetime, we are able to provide definitions of the total energy, the total linear momentum, the total angular momentum, respectively. And we prove two positive mass theorems, corresponding to these two sorts of spatial infinities, for spacelike hypersurfaces whose mean curvatures are bounded by certain constant from above.
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