2019
DOI: 10.3934/cpaa.2019075
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On the existence of solutions and causality for relativistic viscous conformal fluids

Abstract: We consider a stress-energy tensor describing a pure radiation viscous fluid with conformal symmetry introduced in [3]. We show that the corresponding equations of motions are causal in Minkowski background and also when coupled to Einstein's equations, and solve the associated initial-value problem.

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Cited by 14 publications
(25 citation statements)
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“…Therefore, we have verified the hypotheses of [56, Theorem A.23] and we conclude that equations (3) admit a solution in a neighborhood of p. Recall that a solution to Einstein's equations in wave coordinates gives rise to a solution to the full Einstein equations (i.e., Einstein's equations in arbitrary coordinates) if and only if the constraint equations are satisfied, which is the case by assumption. Thus, we have obtained a solution to Einstein's equations coupled to (1) in a neighborhood of p. A standard gluing argument that relies on the causality of solutions already established (see, e.g., [9,Chapter 10] or [56]) gives a solution defined in a neighborhood of Σ. We have therefore obtained a space-time where statements (1)-(5) hold (we notice that statements (2)-(4) are immediate consequences of the 22 above constructions).…”
Section: Appendix A: Kinetic Theory Derivationmentioning
confidence: 99%
“…Therefore, we have verified the hypotheses of [56, Theorem A.23] and we conclude that equations (3) admit a solution in a neighborhood of p. Recall that a solution to Einstein's equations in wave coordinates gives rise to a solution to the full Einstein equations (i.e., Einstein's equations in arbitrary coordinates) if and only if the constraint equations are satisfied, which is the case by assumption. Thus, we have obtained a solution to Einstein's equations coupled to (1) in a neighborhood of p. A standard gluing argument that relies on the causality of solutions already established (see, e.g., [9,Chapter 10] or [56]) gives a solution defined in a neighborhood of Σ. We have therefore obtained a space-time where statements (1)-(5) hold (we notice that statements (2)-(4) are immediate consequences of the 22 above constructions).…”
Section: Appendix A: Kinetic Theory Derivationmentioning
confidence: 99%
“…For brevity, our proof will omit certain technicalities that might be of interest for more mathematically minded readers but would obfuscate the main ideas. Those interested in such technical aspects can consult [107], where proofs of Theorems 1 and 2 are given for an audience of mathematically inclined readers 18 . Proof of Theorem 1.…”
Section: Well-posedness and Causalitymentioning
confidence: 99%
“…In[107], for simplicity, only the case a 1 = 4, a 2 ≥ 3a 1 a 1 −1 = 4 is treated. The arguments there presented, however, are essentially the same to cover the remaining cases.…”
mentioning
confidence: 99%
“…The characteristics corresponding to u α ξ α = 0 are simply the flow lines of u α , which are causal as long as u α remains timelike. The characteristics associated with the vanishing of the bracket in (7) are precisely the characteristics of an acoustical metric [55,72] with an effective sound speed squared given by c 2 acoustical = ζ τΠ(ε+P +Π) + α 1 + α2 n ε+P +Π ≥ 0. Thus, the system will be causal as long as u α remains timelike (and normalized) and c 2 acoustical ≤ 1, which is precisely condition (1).…”
mentioning
confidence: 99%