2016
DOI: 10.1088/0264-9381/33/20/205002
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Generalised hyperbolicity in spacetimes with string-like singularities

Abstract: In this paper we present well-posedness results for H 1 solutions of the wave equation for spacetimes that contain string-like singularities. These results extend a framework in which one characterises gravitational singularities as obstruction to the dynamics of test fields rather than point particles. In particular, we discuss spacetimes with cosmic strings.

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Cited by 5 publications
(8 citation statements)
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References 33 publications
(52 reference statements)
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“…Since then, these requirements have been progressively reduced to the requirement that the second partial weak derivatives of g ab be square integrable and of K ab once differentiable [61][62][63][64][65][66][67][68]; the precise statement is that g ab is in the Sobolev space H 3/2+ loc and K ab in H 1/2+ loc for > 0. More recently, studies of low-regularity metrics in the context of junction conditions have produced limited proofs of local well-posedness for metrics with only first partial weak derivatives being square integrable: g ab ∈ H 1 loc and K ab ∈ H 0 loc [69][70][71][72][73]. This is precisely the regularity regime of our desired results, and we will assume existence, in accordance with expectations partially borne out in this class of cases for the Cauchy problem.…”
Section: Multiple Junctionsmentioning
confidence: 99%
“…Since then, these requirements have been progressively reduced to the requirement that the second partial weak derivatives of g ab be square integrable and of K ab once differentiable [61][62][63][64][65][66][67][68]; the precise statement is that g ab is in the Sobolev space H 3/2+ loc and K ab in H 1/2+ loc for > 0. More recently, studies of low-regularity metrics in the context of junction conditions have produced limited proofs of local well-posedness for metrics with only first partial weak derivatives being square integrable: g ab ∈ H 1 loc and K ab ∈ H 0 loc [69][70][71][72][73]. This is precisely the regularity regime of our desired results, and we will assume existence, in accordance with expectations partially borne out in this class of cases for the Cauchy problem.…”
Section: Multiple Junctionsmentioning
confidence: 99%
“…Proof. The results of [5,6,7] establish well-posedness. The only thing that remains to be shown is that the weak solutions have the correct support.…”
Section: The Lapse Function N Can Be Chosen Asmentioning
confidence: 87%
“…Proof The main idea is to use Galerkin's method. We sketch the proof below for a complete proof see [5,6,7].…”
Section: The Lapse Function N Can Be Chosen Asmentioning
confidence: 99%
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“…It also ensures that the solutions to the wave equation are in H 2 loc (M ) (see Appendix B for details of the function spaces we use) as shown in Theorem 4.7 below, which ensures we have enough regularity to define the quantisation functors we need. Although one can define solutions to the wave equation for metrics of lower regularity [51,52] there are difficulties in defining the corresponding advanced and retarded Green operators for these cases. In Section 3 we establish the results we need to prove existence and uniqueness of solutions to the forward (and backward) initial value problem for the wave equation on R n+1 for C 1,1 metrics.…”
Section: Introductionmentioning
confidence: 99%