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Phys. Rev. D 53, 4327–4334 (1996)

Einstein’s equations and the chiral model

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Viqar Husain
Department of Mathematics and Statistics, University of Calgary, Calgary, Alberta, Canada T2N 4N1
Center for Gravitational Physics and Geometry, Department of Physics, The Pennsylvania State University, University Park, Pennsylvania 16802-6300

Received 3 August 1995; published in the issue dated 15 April 1996

The vacuum Einstein equations for spacetimes with two commuting spacelike Killing field symmetries are studied using the Ashtekar variables. The case of compact spacelike hypersurfaces which are three-tori is considered, and the determinant of the Killing two-torus metric is chosen as the time gauge. The Hamiltonian evolution equations in this gauge may be rewritten as those of a modified SL(2) principal chiral model with a time-dependent ‘‘coupling constant,’’ or equivalently, with time-dependent SL(2) structure constants. The evolution equations have a generalized zero-curvature formulation. Using this form, the explicit time dependence of an infinite number of spatial-diffeomorphism-invariant phase-space functionals is extracted, and it is shown that these are observables in the sense that they Poisson commute with the reduced Hamiltonian. An infinite set of observables that have SL(2) indices is also found. This determination of the explicit time dependence of an infinite set of spatial-diffeomorphism-invariant observables amounts to the solutions of the Hamiltonian Einstein equations for these observables. © 1996 The American Physical Society.

© 1996 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.53.4327
DOI:
10.1103/PhysRevD.53.4327
PACS:
04.20.Fy, 04.20.Cv, 04.60.Ds