11.07.2015 Views

International Congress of Mathematicians

International Congress of Mathematicians

International Congress of Mathematicians

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Mass and Scalar Curvature 233Schwarzschild spacetime amongst static metrics with smooth black hole boundary[13], which we briefly outline.A static spacetime is a Lorentzian 4-manifold with a hypersurface-orthogonaltimelike Killing vector. With V denoting the length <strong>of</strong> the Killing vector, the metricg on the spacelike hypersurface satisfies the static equationsRiCg = V~ l V 2 V, ( .{A g V = 0.'Smoothness implies the boundary set S = {V = 0} is totally geodesic; analyticity<strong>of</strong> g, V can be used to show the asymptotic expansions9ij = (1 + 2m/r)% + 0(r- 2 ),V = 1 — m/r + 0(r~ 2 ),as r —t oo for some constant m £ R. The metrics g ± = 4 g where = ± on the two copies <strong>of</strong> M, gives a complete AF manifold with R(g) = 0 andvanishing mass. The PMT shows (M, g) is flat and it follows without difficulty that(M,g) is Schwarzschild. This extends previous results [31, 43] which required theboundary to be connected.2. Penrose conjectureA boundary component S with mean curvature F = 0 is called a black hole orhorizon, since if (M, g) is a totally geodesic hypersurface then S is a trapped surfaceand hence, by the Penrose singularity theorem [26], lies within an event horizon andis destined to encounter geodesic incompleteness in the predictable future.The spatial Schwarzschild metric g = 1_' 2 M/ r + r 2 (d'à 2 + sin édtp 2 ) with M < 0shows that the completeness condition in the PMT is important, but it can beweakened to allow horizon boundary components <strong>of</strong> M. This follows immediatelyfrom the minimal surface argument [45]; or by an extension to the Witten argument[22], imposing one <strong>of</strong> the boundary conditionsip = ±eip on S = dM, (2.1)on the spinor field tp, where e = 7"7° satisfies e 2 = 1. An interesting extension isobtained by imposing the spectral boundary conditionP+'ip = 0 on S (2.2)where F + is the projection onto the subspace <strong>of</strong> positive eigenspinors <strong>of</strong> the inducedDirac operator T>-£. Using the remarkable Hijazi-Bär estimate [28, 2]|A| > V47r/|S|, (2.3)for the eigenvalues <strong>of</strong> VY. when S ~ S 2 , Herzlich showed [27]

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