Quasi-local energy-momentum and two-surface characterization of the pp-wave spacetimes
arXiv:gr-qc/9512013 · doi:10.1088/0264-9381/13/6/028
Abstract
In the present paper the determination of the {\it pp}-wave metric form the geometry of certain spacelike two-surfaces is considered. It has been shown that the vanishing of the Dougan--Mason quasi-local mass , associated with the smooth boundary of a spacelike hypersurface , is equivalent to the statement that the Cauchy development is of a {\it pp}-wave type geometry with pure radiation, provided the ingoing null normals are not diverging on and the dominant energy condition holds on . The metric on itself, however, has not been determined. Here, assuming that the matter is a zero-rest-mass-field, it is shown that both the matter field and the {\it pp}-wave metric of are completely determined by the value of the zero-rest-mass-field on and the two dimensional Sen--geometry of provided a convexity condition, slightly stronger than above, holds. Thus the {\it pp}-waves can be characterized not only by the usual Cauchy data on a {\it three} dimensional but by data on its {\it two} dimensional boundary too. In addition, it is shown that the Ludvigsen--Vickers quasi-local angular momentum of axially symmetric {\it pp}-wave geometries has the familiar properties known for pure (matter) radiation.
15 pages, Plain Tex, no figures
References in corpus (5)
Cited by in corpus (8)
- Canonical Quasilocal Energy and Small Spheres
- On the roots of the Poincare structure of asymptotically flat spacetimes
- On certain quasi-local spin-angular momentum expressions for small spheres
- On certain quasi-local spin-angular momentum expressions for large spheres near the null infinity
- Black Hole Interaction Energy
- Mass, gauge conditions and spectral properties of the Sen-Witten and 3-surface twistor operators in closed universes
- Quasi-local gravitational angular momentum and centre of mass from generalised Witten equations
- Quasi-local holography and quasi-local mass of classical fields in Minkowski spacetime