In this article, I discuss the construction of some globally conserved currents that one can construct in the absence of a Killing vector. One is based on the Komar current, which is constructed from an arbitrary vector field and has an identically vanishing divergence. I obtain some expressions for Komar currents constructed from some generalizations of Killing vectors which may in principle be constructed in a generic spacetime. I then present an explicit example for an outgoing Vaidya spacetime which demonstrates that the resulting Komar currents can yield conserved quantities that behave in a manner expected for the energy contained in the outgoing radiation. Finally, I describe a method for constructing another class of (non-Komar) globally conserved currents using a scalar test field that satisfies an inhomogeneous wave equation, and discuss two examples; the first example may provide a useful framework for examining the arrow of time and its relationship to energy conditions, and the second yields (with appropriate initial conditions) a globally conserved energy-and momentumlike quantity that measures the degree to which a given spacetime deviates from symmetry.
I. THE KOMAR CURRENTIn a 1959 article [1], Arthur Komar presented a globally conserved current (the Komar current) for general relativistic spacetimes, which is constructed from an arbitrary vector field U µ (which serves as the generator for diffeomorphisms). The Komar current is of the form: 1(1)The Komar current has theoretical appeal because it can be derived from the action in the context of Noether's theorem-in [2][3][4], it was shown that the Komar current is in fact the conserved current corresponding to the diffeomorphism invariance of the Einstein-Hilbert Lagrangian coupled to matter. 2 Using the Ricci identity [∇ µ , ∇ ν ]T αβ = R α σµν T σβ + R β σµν T ασ for the Levi-Civita connection ∇ µ , it is straightforward to show that the divergence of J µ K identically vanishes:The above result is an identity for any quantity of the form given in Eq. (1); it only depends on the Ricci identity for rank-2 tensors. Note also that Eq. (2) permits a shift freedom in J µ K ; any divergence-free vector added to J µ K preserves the divergence-free property Eq. (2). One potentially useful example is a vector field of the form 1 Note that there is a gauge freedom in this definition; for a torsionfree connection ∇µ, J µ K is invariant under the transformation U µ → U µ + ∇ µ σ (σ being a scalar field). 2 I also refer the reader to [5] and related work which extend the analysis to more general theories of gravity [6][7][8].∇ µ φ, which is divergence free if the scalar field satisfies the wave equation φ = 0. From the Komar current J µ K , I may construct the 3form:By Stokes' theorem, the integral of the above over some constant-time hypersurface Σ t becomes:where dΣ µ and dS µν are the respective surface elements 3 for Σ t and ∂Σ t . Equation (4) may be used to construct quasilocal expressions for quantities associated with a Komar current. Note in a close...