2019
DOI: 10.4171/rmi/1130
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Weighted fractional chain rule and nonlinear wave equations with minimal regularity

Abstract: We consider the local well-posedness for 3-D quadratic semi-linear wave equations with radial data:It has been known that the problem is well-posed for s ≥ 2 and ill-posed for s < 3/2. In this paper, we prove unconditional well-posedness up to the scaling invariant regularity, that is to say, for s > 3/2 and thus fill the gap which was left open for many years. For the purpose, we also obtain a weighted fractional chain rule, which is of independent interest. Our method here also works for a class of nonlinear… Show more

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Cited by 10 publications
(6 citation statements)
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“…it turns out that the homogeneous local energy and KSS-type estimates are available (see Metcalfe-Sogge [22] and Hidano-Wang-Yokoyama [10, Lemma 2.3]). Thus, in spirit of [9] and [7], we could prove well-posed results for the problem with c 2 = 0 in the radial case, with sharp lower bound of the lifespan.…”
Section: Introductionmentioning
confidence: 76%
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“…it turns out that the homogeneous local energy and KSS-type estimates are available (see Metcalfe-Sogge [22] and Hidano-Wang-Yokoyama [10, Lemma 2.3]). Thus, in spirit of [9] and [7], we could prove well-posed results for the problem with c 2 = 0 in the radial case, with sharp lower bound of the lifespan.…”
Section: Introductionmentioning
confidence: 76%
“…These nonlinear estimates are well-known, see, e.g., [9] and [7]. For reader's convenience, we give a proof of (2.12) here.…”
Section: 2mentioning
confidence: 88%
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“…It should be mentioned that improvement of regularity in the presence of radial symmetry was first observed in [18] for semilinear equations such as ✷u = c 1 (∂ t u) 2 + c 2 |∇u| 2 . (See also page 176 of [31], Section 5 of [25], and [9], [30], and [6] for related results.) We also mention that it was also observed for the wave equation with a power-type nonlinear term ✷u = F (u), first by Lindbald and Sogge [23], and then by some authors (see [4], [12], [3]), and quasilinear wave equations of the form ∂ 2 t u − a 2 (u)∆u = c 1 (∂ t u) 2 + c 2 |∇u| 2 , by [7] and [41].…”
Section: Introduction and Main Resultsmentioning
confidence: 99%