2009
DOI: 10.4310/cag.2009.v17.n1.a3
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Large-sphere and small-sphere limits of the Brown-York mass

Abstract: In this paper, we will study the limiting behavior of the Brown-York mass of the coordinate spheres in an asymptotically flat manifold. Limiting behaviors of volumes of regions related to coordinate spheres are also obtained, including a discussion on the isoperimetric mass introduced by Huisken [13]. We will also study expansions of the Brown-York mass and the Hawking mass of geodesic spheres with center at a fixed point p of a three manifold. Some geometric consequences will be derived.

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Cited by 77 publications
(76 citation statements)
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“…Here the center-of-mass integral is also given in terms of a charge integral of the curvature. The large sphere limit of the energy for metrics with the weakest possible falloff conditions is calculated in [181, 462]. A further demonstration that the spatial infinity limit of the Brown-York energy in an asymptotically Schwarzschild spacetime is the ADM energy is given in [180].…”
Section: The Hamilton-jacobi Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…Here the center-of-mass integral is also given in terms of a charge integral of the curvature. The large sphere limit of the energy for metrics with the weakest possible falloff conditions is calculated in [181, 462]. A further demonstration that the spatial infinity limit of the Brown-York energy in an asymptotically Schwarzschild spacetime is the ADM energy is given in [180].…”
Section: The Hamilton-jacobi Methodsmentioning
confidence: 99%
“…On the other hand, the special light cone reference used in [118, 335] reproduces the expected result in nonvacuum, and yields [1/(90 G )] r 5 T abcd t a t b t c t d in vacuum. The small sphere limit was also calculated in [181] for small geodesic spheres in a time symmetric spacelike hypersurface.…”
Section: The Hamilton-jacobi Methodsmentioning
confidence: 99%
“…Let g r be the induced metric on S r and letg r = r −2 g r . Identifying S r with S 2 = { |y| = 1} via a map y = r −1 x, one can deduce from (6.3) that g r − σ C 3 ≤ Cr −τ (6.4) (see (2.17) in [18] for instance). Here σ is the standard metric on S 2 with area 4π and C > 0 is a constant independent on r.…”
Section: Limits Along Isomeric Embeddings Of Large Spheres Into Schwamentioning
confidence: 99%
“…By (6.9), Let V (r) be the volume of the region enclosed by S r in (M,g). By (2.28) in [18], (6.24) V (r) = 1 2 rA(r) − 2 3 πr 3 + 2πmr 2 + o(r 2 ).…”
Section: 2mentioning
confidence: 99%
“…where H g 0 denotes the mean curvature of Σ c when embedded, with its induced metric γ c , into (R 3 , g 0 ). The right hand side is the Brown-York mass of Σ c and, by [35,12], it converges to m ADM (M, g) as c → 1. This recovers Bray's capacity inequality (1.2).…”
Section: )mentioning
confidence: 99%