2018
DOI: 10.1103/physrevd.97.084053
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Conformal and covariant Z4 formulation of the Einstein equations: Strongly hyperbolic first-order reduction and solution with discontinuous Galerkin schemes

Abstract: We present a strongly hyperbolic first-order formulation of the Einstein equations based on the conformal and covariant Z4 system (CCZ4) with constraint-violation damping, which we refer to as FO-CCZ4. As CCZ4, this formulation combines the advantages of a conformal and traceless formulation, with the suppression of constraint violations given by the damping terms, but being first order in time and space, it is particularly suited for a discontinuous Galerkin (DG) implementation. The strongly hyperbolic first-… Show more

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Cited by 54 publications
(86 citation statements)
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References 97 publications
(249 reference statements)
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“…1 for both simulations. For comparison, we also show the results obtained with the original FO-CCZ4 system [35] without curl cleaning. One can observe that the new hyperbolic GLM curl cleaning proposed in this paper reduces the errors in the Hamiltonian constraint by two orders of magnitude.…”
Section: Robust Stability Testmentioning
confidence: 99%
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“…1 for both simulations. For comparison, we also show the results obtained with the original FO-CCZ4 system [35] without curl cleaning. One can observe that the new hyperbolic GLM curl cleaning proposed in this paper reduces the errors in the Hamiltonian constraint by two orders of magnitude.…”
Section: Robust Stability Testmentioning
confidence: 99%
“…We run this test problem with two different setups. First, the standard FO-CCZ4 system [35] with the default choice e = 1, c = 1, κ i = 0 and without GLM curl cleaning is used. Then we run the same test problem again with GLM curl cleaning, using the cleaning speeds e = 2, a A c = a P c = a D c = a A d = a P d = a D d = 1.5, the damping parameters A c = P c = D c = A d = P d = D d = 1 and c = 0, κ i = 0.…”
Section: Wavefield Generated By Two Rotating Massesmentioning
confidence: 99%
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“…Finally, we presented a 3+1 split of the governing equations in Sec. 5.1 which are then solved using the ADER-DG family of high-order numerical schemes [14,15,16,38,37] designed specifically for hyperbolic partial differential equations, see Sec. 5.…”
Section: Numerical Examplesmentioning
confidence: 99%
“…Only after adding suitable first and second order ordering constraints, which arise from the definition of the auxiliary variables, it is possible to obtain a provably strongly hyperbolic and thus well-posed evolution system, denoted by FO-CCZ4 in the following. For all details of the derivation, the strong hyperbolicity proof and numerical results achieved with high order ADER-DG schemes, the reader is referred to [126]. In order to give an idea about the complexity of the Einstein field equations, it should be mentioned that one single evaluation of the FO-CCZ4 system requires about 20,000 floating point operations!…”
Section: A Strongly Hyperbolic First Order Reduction Of the Ccz4 Formmentioning
confidence: 99%