Fully constrained, high-resolution shock-capturing, formulation of the Einstein-fluid equations in dimensions
arXiv:2103.04435 · doi:10.1103/PhysRevD.104.024061
Abstract
Four components of the axisymmetric Einstein equations in 2+1 dimensions with negative cosmological constant can be written as and , where the dots stand for stress-energy terms, and and are scalars. In vacuum, they reduce to the constant mass and angular momentum parameters of the BTZ solution of the same name. The integrability conditions for the Einstein equations give rise to two conserved stress-energy currents and . The angular momentum current is just the Noether current due to axisymmetry, but the mass current is unexpected in the presence of rotation. The conserved quantity exists in all dimensions in spherical symmetry, known as the Misner-Sharp, Hawking or Kodama mass, but in 2+1 dimensions exists also in axisymmetry, even with rotation. We use and to give a fully constrained formulation of the axisymmetric Einstein equations in 2+1 dimensions, where the Einstein equations are solved by explicit integration from the center along time slices. We use the two conserved matter currents in the construction of a high-resolution shock-capturing formulation of the Einstein-perfect fluid system, in which and momentum are then exactly conserved by construction. We demonstrate convergence of the code in the test cases of generic dispersion and collapse and stable and unstable rotating stars.
arXiv comment23 pages, 17 figures, Typos corrected. This version has been accepted by PRD
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Cited by in corpus (5)
- Extension of Kodama vector and quasilocal quantities in three-dimensional axisymmetric spacetimes
- Geometrical origin of the Kodama vector
- Charged rotating BTZ solution revisited: New coordinates and algebraic classifications
- Critical collapse of an axisymmetric ultrarelativistic fluid in dimensions
- Extremal rotating BTZ black holes cannot be dressed in (anti-)self-dual Maxwell field