A Penrose-type inequality for static spacetimes
Brian Harvie
TL;DR
This work proves a Penrose-type lower bound on the mass of asymptotically flat static triples under the timelike convergence condition, namely $m \ge \frac{1}{2} \left( \frac{|\Sigma|}{w_{n-1}} \right)^{\frac{n-2}{n-1}} - \frac{1}{2(n-1) w_{n-1}} \int_{\Sigma} V H\,d\sigma$, with equality characterizing a Schwarzschild region. The authors introduce a monotone quantity $Q(t)$ along inverse mean curvature flow, show its non-increase under both smooth and weak IMCF, and derive a flux bound for $V$ from the mass formula, all under the timelike convergence condition. The results extend Minkowski-type and Penrose-type inequalities to higher-dimensional static spacetimes and yield a rigidity statement: equality forces the geometry to be Schwarzschild; this also provides a Riemannian Penrose-type inequality for static spaces in all dimensions under TCC. Overall, the paper provides a robust geometric-analytic framework linking mass, horizon geometry, and static vacuum rigidity in higher-dimensional general relativity.
Abstract
We establish a lower bound on the total mass of the time slices of (n + 1)-dimensional asymptotically flat standard static spacetimes under the timelike convergence condition. The inequality can be viewed equivalently as a Minkowski-type inequality in these spaces, i.e. as a lower bound on the total mean curvature of the boundary, and thus extends inequalities from [3], [22], [19], and [10]. Equality is achieved only by slices of Schwarzschild space and is related to the characterization of quasi-spherical static vacuum metrics from [10]. As a notable special case of the main inequality, we obtain the Riemannian Penrose inequality in all dimensions for static spaces under the TCC.
