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A well-balanced discontinuous Galerkin method for the first-order Z4 formulation of the Einstein-Euler system.

, , , and . CoRR, (2023)

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ADER-WENO finite volume schemes with space-time adaptive mesh refinement., , , and . J. Comput. Phys., (2013)A well-balanced discontinuous Galerkin method for the first-order Z4 formulation of the Einstein-Euler system., , , and . J. Comput. Phys., (2024)Very high order PNPM schemes on unstructured meshes for the resistive relativistic MHD equations., and . J. Comput. Phys., 228 (18): 6991-7006 (2009)High order cell-centered Lagrangian-type finite volume schemes with time-accurate local time stepping on unstructured triangular meshes., , and . J. Comput. Phys., (2015)Space-time adaptive ADER-DG schemes for dissipative flows: Compressible Navier-Stokes and resistive MHD equations., , and . Comput. Phys. Commun., (2017)High order ADER schemes for a unified first order hyperbolic formulation of Newtonian continuum mechanics coupled with electro-dynamics., , , and . J. Comput. Phys., (2017)High order ADER schemes for a unified first order hyperbolic formulation of continuum mechanics: Viscous heat-conducting fluids and elastic solids., , , and . J. Comput. Phys., (2016)A high order special relativistic hydrodynamic and magnetohydrodynamic code with space-time adaptive mesh refinement., and . Comput. Phys. Commun., (2015)ADER-WENO Finite Volume Schemes with Space-Time Adaptive Mesh Refinement, , , and . CoRR, (2012)A posteriori subcell limiting of the discontinuous Galerkin finite element method for hyperbolic conservation laws., , , and . J. Comput. Phys., (2014)