2015
DOI: 10.48550/arxiv.1504.00687
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Stable fixed points of the Einstein flow with positive cosmological constant

Abstract: We prove nonlinear stability for a large class of solutions to the Einstein equations with a positive cosmological constant and compact spatial topology in arbitrary dimensions, where the spatial metric is Einstein with either positive or negative Einstein constant. The proof uses the CMC Einstein flow and stability follows by an energy argument. We prove in addition that the development of non-CMC initial data close to the background contains a CMC hypersurface, which in turn implies that stability holds for … Show more

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Cited by 7 publications
(14 citation statements)
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“…Thus the smallness of R 0ij + 2g 0ij H 3 (Σ,g 0 ) implies smallness for g 0ij − γ ij H 5 (Σ,γ) and hence the rescaled version of (1.3) entails that g 0ij −γ ij H 5 (Σ,γ) + k 0ij +γ ij H 4 (Σ,γ) ε. Now we can prove along the lines of the corresponding argument presented in [29,15] to show the existence of a CMC surface in the non vacuum setting. Therefore, the data in Theorem 1.1 can be generalized to be non-CMC.…”
mentioning
confidence: 88%
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“…Thus the smallness of R 0ij + 2g 0ij H 3 (Σ,g 0 ) implies smallness for g 0ij − γ ij H 5 (Σ,γ) and hence the rescaled version of (1.3) entails that g 0ij −γ ij H 5 (Σ,γ) + k 0ij +γ ij H 4 (Σ,γ) ε. Now we can prove along the lines of the corresponding argument presented in [29,15] to show the existence of a CMC surface in the non vacuum setting. Therefore, the data in Theorem 1.1 can be generalized to be non-CMC.…”
mentioning
confidence: 88%
“…(1.4)- (1.5) for the rescaling). To match the condition in [15], one needs the smallness for g 0 − γ H s (Σ,γ) + k 0 + γ H s−1 (Σ,γ) , s > 3/2 + 1, where γ is the hyperbolic metric. We take s = 5 and choose the harmonic coordinates with respect to g 0 and γ.…”
mentioning
confidence: 99%
“…Considering sufficiently small initial data which is not necessarily CMC, the maximal globally hyperbolic development under the Einstein-Vlasov system is, locally in time, as close to the background geometry as desired in a suitable regularity [Ri]. The existence of a CMC surface in such a spacetime can be shown along the lines of the corresponding argument in the vacuum case presented for instance in [FK15]. 10.3.…”
Section: Global Existence and Completenessmentioning
confidence: 99%
“…With the spacetime topology of R × M , one has the freedom to choose the spatial slice as long as it is diffeomorphic to a Cauchy hypersurface. Let M be a Cauchy hypersurface with an induced metric g which together with (k, N, X) satisfies the Einstein evolution and constraint equations (7)(8)(9)(10). Now let φ be a an element of the identity component of the diffeomorphism group (D 0 ) of M .…”
Section: Field Equations and Gauge Fixingmentioning
confidence: 99%
“…In the case of '2+1' Einstein flow on R × S genus with genaus > 1, Teichmüller space plays the role of the Einstein moduli space and special techniques [3,12] are used to study the global existence (by utilizing the properness of the Dirichlet energy functional defined on the Teichmüller space). Recently [9] studied the Lyapunov stability of these background solutions including a positive cosmological constant. However, in order to establish the 'attractor' property of the background solutions, it is necessary to prove the asymptotic stability.…”
mentioning
confidence: 99%