Abstract

We propose a new foliation of asymptotically Euclidean initial data sets by 2-spheres of constant spacetime mean curvature (STCMC). The leaves of the foliation have the STCMC-property regardless of the initial data set in which the foliation is constructed which asserts that there is a plethora of STCMC 2-spheres in a neighborhood of spatial infinity of any asymptotically flat spacetime. The STCMC-foliation can be understood as a equivariant relativistic generalization of the CMC-foliation suggested by Huisken and Yau (Invent Math 124:281–311, 1996). We show that a unique STCMC-foliation exists near infinity of any asymptotically Euclidean initial data set with non-vanishing energy which allows for the definition of a new notion of total center of mass for isolated systems. This STCMC-center of mass transforms equivariantly under the asymptotic Poincaré group of the ambient spacetime and in particular evolves under the Einstein evolution equations like a point particle in Special Relativity. The new definition also remedies subtle deficiencies in the CMC-approach to defining the total center of mass suggested by Huisken and Yau (Invent Math 124:281–311, 1996) which were described by Cederbaum and Nerz (Ann Henri Poincaré 16:1609–1631, 2015).

Highlights

  • Introduction and goalsIn General Relativity, isolated systems are individual or clusters of stars, black holes, or galaxies that do not interact with any matter or gravitational radiation outside the system under consideration

  • We suggest a definition of total center of mass for suitably isolated systems and argue that this center of mass notion behaves as a point particle in Special Relativity in a suitable sense

  • Because of the spacetime geometry nature of the spacetime constant mean curvature (STCMC)-condition, we expect that STCMC-surfaces and STCMC-foliations will have a number of applications beyond the definition of a center of mass of an isolated system as well as beyond the setting of asymptotically Euclidean initial data sets

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Summary

Introduction and goals

In General Relativity, isolated (gravitating) systems are individual or clusters of stars, black holes, or galaxies that do not interact with any matter or gravitational radiation outside the system under consideration. The analytic techniques in our proofs rely on and unify and simplify those developed by Metzger [35] and Nerz [40,41] Concluding this introduction, we would like to point out that the notion of spacetime mean curvature of 2-surfaces in initial data sets has independently been considered in other contexts, both before and after the results of this paper had been announced. Because of the spacetime geometry nature of the STCMC-condition, we expect that STCMC-surfaces and STCMC-foliations will have a number of applications beyond the definition of a center of mass of an isolated system as well as beyond the setting of asymptotically Euclidean initial data sets.

Preliminaries
Center of mass
Miscellannea
Strategy of the proofs of Theorems 2 and 4
A priori estimates on STCMC-surfaces
The linearization of spacetime mean curvature
Invertibility of the operator L
Existence and uniqueness of the STCMC-foliation
Existence of the STCMC-foliation
Let 0 smooth
Uniqueness of STCMC-surfaces
The coordinate center of the STCMC-foliation
A variational formula for STCMC-surfaces
STCMC-center of mass
Evolution
Poincaré-equivariance and accordance with Special Relativity
A concrete graphical example in the Schwarzschild spacetime
Full Text
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