1993
DOI: 10.1215/s0012-7094-93-07103-7
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On the asymptotic behavior of spherically symmetric wave maps

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Cited by 73 publications
(123 citation statements)
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“…On the other hand, Theorem 3.2 below gives actually r^ = z/2 for wave-maps on 2 + 1 dimensional Minkowski space-time. We note that the 2 + 1 dimensional wave map equation is related to the vacuum Einstein equations with cylindrical symmetry {cf eg [8,19,20]). …”
Section: Ee^m^' (I-3)mentioning
confidence: 99%
“…On the other hand, Theorem 3.2 below gives actually r^ = z/2 for wave-maps on 2 + 1 dimensional Minkowski space-time. We note that the 2 + 1 dimensional wave map equation is related to the vacuum Einstein equations with cylindrical symmetry {cf eg [8,19,20]). …”
Section: Ee^m^' (I-3)mentioning
confidence: 99%
“…A considerable amount of the literature is devoted to problems with certain symmetry properties, such as radial or equivariant maps. We mention for instance [6], [7], [27], [30], [33], [35] where various fundamental aspects like local and global well-posedness, asymptotic behavior or blow up are studied. At the end of the 1990s new techniques were developed, capable of treating the full system without symmetry assumptions.…”
Section: Introductionmentioning
confidence: 99%
“…Hence by (1.9), we have Γ L 4 (R 4 ) ε. Using the Sobolev embeddingḢ 1 (R 4 ) ֒→ L 4 (R 4 ) and the above inequalities we have…”
Section: Linear Dispersive Estimates For Wave Equations On a Curved Bmentioning
confidence: 87%
“…Also in the appendix, Section 9.1, we show that the "covariant" Sobolev spaceṡ H s (M ; N ), with (M, g) = (R 4 , g) with the metric g as in (1.8)-(1.11) are equivalent to the "flat" spacesḢ s ((R 4 , g 0 ); N ) with the Euclidean metric g 0 on R 4 . Hence in what follows we can, when convenient, ignore the non-Euclidean metric g for the purpose of estimating Sobolev norms, replacing covariant derivatives on M with partial derivatives and the volume form dvol g with the Euclidean volume form.…”
mentioning
confidence: 87%