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Geometric relationship between the generalized Komar energy and the Arnowitt-Deser-Misner mass in dynamical spacetimes

Zhi-Wei Wang1,2,* and Samuel L. Braunstein2,†

  • *Contact author: zhiweiwang.phy@gmail.com
  • †Contact author: sam.braunstein@york.ac.uk

Phys. Rev. D 114, 024079 – Published 28 July, 2026

DOI: https://doi.org/10.1103/nl77-bv95

Abstract

The standard Komar mass provides an elegant, quasilocal measure of total gravitating energy for stationary spacetimes, but it conventionally fails in dynamical scenarios that lack an exact global timelike Killing vector field. In this paper, we explore a generalized Komar energy integral bounded by a spacelike two-surface, obtained by replacing the Killing vector with the purely kinematic normal evolution vector field ξμ=NT^μ associated with a 3+1 spacelike foliation. Through a step-by-step mathematical derivation, we show that this generalized integral reduces to the spatial boundary flux of the Eulerian four-acceleration. Furthermore, by evaluating the asymptotic vacuum constraints in generic dynamical spacetimes without restricting the metric to an isotropic or transverse-traceless spatial gauge, we establish, at leading asymptotic order, a relationship mapping this flux to the global Arnowitt-Deser-Misner (ADM) mass. By constructing a superpotential for the linearized spatial Einstein tensor, we prove that the dynamically generalized Komar energy and the ADM mass are equivalent up to a boundary flux of the temporal evolution of the conjugate momentum. We verify this relationship through nontrivial analytical test cases involving dynamical gauge foliations and physical gravitational wave radiation, revealing that the geometric momentum flux isolates longitudinal time-slicing artifacts while naturally decoupling from transverse radiative degrees of freedom.

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