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Relativistic dissipative fluids in the trace-fixed particle frame: Strongly hyperbolic quasi-linear first-order evolution equations

J. Félix Salazar, Ana Laura García-Perciante, Olivier Sarbach

TL;DR

The paper develops a fully nonlinear, relativistic dissipative fluid theory in the trace-fixed particle (TFP) frame, ensuring causality and stability by proving strong hyperbolicity of a first-order quasilinear reformulation. By introducing auxiliary gradient fields and constraints, the authors construct a constrained system whose principal symbol decomposes into scalar, vector, and tensor blocks and admits smooth, state-dependent symmetrizers. They explicitly diagonalize the blocks under a key set of conditions, derive a consistent constraint propagation system, and prove local well-posedness of the Cauchy problem for the nonlinear system. The framework preserves thermodynamic consistency, aligns with the second law, and provides a tractable, well-posed model suitable for numerical relativity and high-energy astrophysical contexts.

Abstract

In this paper we derive a new first-order theory of relativistic dissipative fluids by adopting the trace-fixed particle frame. Whereas in a companion letter we show that this theory is hyperbolic, causal and stable at global equilibrium states, here we prove that the full nonlinear system of equations can be cast into a first-order quasilinear system which is strongly hyperbolic. By rewriting the system in first-order form, auxiliary constraints are introduced. However, we show that these constraints propagate, and thus our theory leads to a well-posed Cauchy problem.

Relativistic dissipative fluids in the trace-fixed particle frame: Strongly hyperbolic quasi-linear first-order evolution equations

TL;DR

The paper develops a fully nonlinear, relativistic dissipative fluid theory in the trace-fixed particle (TFP) frame, ensuring causality and stability by proving strong hyperbolicity of a first-order quasilinear reformulation. By introducing auxiliary gradient fields and constraints, the authors construct a constrained system whose principal symbol decomposes into scalar, vector, and tensor blocks and admits smooth, state-dependent symmetrizers. They explicitly diagonalize the blocks under a key set of conditions, derive a consistent constraint propagation system, and prove local well-posedness of the Cauchy problem for the nonlinear system. The framework preserves thermodynamic consistency, aligns with the second law, and provides a tractable, well-posed model suitable for numerical relativity and high-energy astrophysical contexts.

Abstract

In this paper we derive a new first-order theory of relativistic dissipative fluids by adopting the trace-fixed particle frame. Whereas in a companion letter we show that this theory is hyperbolic, causal and stable at global equilibrium states, here we prove that the full nonlinear system of equations can be cast into a first-order quasilinear system which is strongly hyperbolic. By rewriting the system in first-order form, auxiliary constraints are introduced. However, we show that these constraints propagate, and thus our theory leads to a well-posed Cauchy problem.

Paper Structure

This paper contains 25 sections, 2 theorems, 127 equations.

Key Result

Theorem 1

Assume $e$, $\eta$, $\kappa$, $\zeta$, and $\Gamma_1$ are smooth ($C^\infty$), strictly positive functions of $T$, fulfilling $0 < c_v = \frac{\partial e}{\partial T} < d k_B$ and either $\Gamma_1 < 1$ or $\Gamma_1 > 1$. Let $\Gamma_2$ be given by (Eq:Gamma2) with $h = e + k_B T$, and suppose the in

Theorems & Definitions (3)

  • Theorem 1
  • Lemma 1
  • Definition 1: oR04