2012
DOI: 10.1016/j.matpur.2012.01.007
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The Glassey conjecture with radially symmetric data

Abstract: In this paper, we verify the Glassey conjecture in the radial case for all spatial dimensions, which states that, for the nonlinear wave equations of the form $\Box u=|\nabla u|^p$, the critical exponent to admit global small solutions is given by $p_c=1+\frac{2}{n-1}$. Moreover, we are able to prove the existence results with low regularity assumption on the initial data and extend the solutions to the sharp lifespan. The main idea is to exploit the trace estimates and KSS type estimates.Comment: 28 page

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Cited by 83 publications
(90 citation statements)
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References 25 publications
(42 reference statements)
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“…After that Strauss [51] conjectured that the threshold for dividing blowup phenomena in finite time for arbitrary "positive" small initial value and global existence of small solutions is given by An alternative proof of lifespan estimate with critical case p = p S (N) via Gauss's hypergeometric function can be found in Zhou [61] and Zhou-Han [65]. Similar problem can be found for (1.1) with G = |∂ t u| p (see e.g., John [27], Sideris [49], Masuda [43], Schaeffer [48] Rammaha [45], Agemi [1], Hidano-Tsutaya [17] Tzvetkov [55], Zhou [62] and Hidano-Wang-Yokoyama [18]). The complete picture of the blowup phenomena for small solutions can be summarized as follows:…”
Section: Introductionmentioning
confidence: 75%
“…After that Strauss [51] conjectured that the threshold for dividing blowup phenomena in finite time for arbitrary "positive" small initial value and global existence of small solutions is given by An alternative proof of lifespan estimate with critical case p = p S (N) via Gauss's hypergeometric function can be found in Zhou [61] and Zhou-Han [65]. Similar problem can be found for (1.1) with G = |∂ t u| p (see e.g., John [27], Sideris [49], Masuda [43], Schaeffer [48] Rammaha [45], Agemi [1], Hidano-Tsutaya [17] Tzvetkov [55], Zhou [62] and Hidano-Wang-Yokoyama [18]). The complete picture of the blowup phenomena for small solutions can be summarized as follows:…”
Section: Introductionmentioning
confidence: 75%
“…= n+1 n−1 . We refer to the classical works [19,48,28,47,45,1,12,55,64,13] for the proof of this conjecture, although up to the knowledge of the author the global existence in the supercritical case for the not radial symmetric case in high dimensions is still open. Recently, in [30] a blow-up result for 1 < p ≤ p Gla (n) has been proved for a semilinear damped wave model in the scattering case, that is, when the time-dependent coefficient of the damping term b(t)u t is nonnegative and summable.…”
Section: Introductionmentioning
confidence: 99%
“…Proof. In order to show the validity of (56) and (57) we will employ the definition of weak solution for (12) with a suitable choice of the test functions (φ, ψ) in (52) and (53). If we assume that (u, v) satisfies (8), then, supp u(t, ·), supp v(t, ·) ⊂ B R+t for any t 0.…”
Section: Introduction Of the Functionals For The Critical Casementioning
confidence: 99%