Extrinsic Curvature and the Einstein Constraints
arXiv:gr-qc/0207095 · doi:10.1103/PhysRevD.67.044022
Abstract
The Einstein initial-value equations in the extrinsic curvature (Hamiltonian) representation and conformal thin sandwich (Lagrangian) representation are brought into complete conformity by the use of a decomposition of symmetric tensors which involves a weight function. In stationary spacetimes, there is a natural choice of the weight function such that the transverse traceless part of the extrinsic curvature (or canonical momentum) vanishes.
8 pages, no figures; added new section; significant polishing of text
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