On the global well-posedness of focusing energy-critical inhomogeneous NLS

We consider the focusing energy-critical inhomogeneous nonlinear Schrödinger equation: i u t + Δ u + g | u | p - 1 u = 0 , u ( 0 ) = φ ∈ H ˙ 1 , where 0 ≤ g i ≤ | x | b g ≤ g s , 0 < b < 4 3 , and p = 5 - 2 b . On the road map of Kenig and Merle (Invent Math 166:645–675, 2006), we show the glo...

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Bibliographic Details
Published in:Journal of evolution equations Vol. 20; no. 4; pp. 1349 - 1380
Main Authors: Cho, Yonggeun, Hong, Seokchang, Lee, Kiyeon
Format: Journal Article
Language:English
Published: Cham Springer International Publishing 01-12-2020
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Summary:We consider the focusing energy-critical inhomogeneous nonlinear Schrödinger equation: i u t + Δ u + g | u | p - 1 u = 0 , u ( 0 ) = φ ∈ H ˙ 1 , where 0 ≤ g i ≤ | x | b g ≤ g s , 0 < b < 4 3 , and p = 5 - 2 b . On the road map of Kenig and Merle (Invent Math 166:645–675, 2006), we show the global well-posedness and scattering of radial solutions under energy condition E g ( φ ) < E g ( Q b ) , and g s 1 p 0 ‖ φ ‖ H ˙ 1 2 < ‖ Q b ‖ H ˙ 1 2 , where Q b is the solution of Δ Q b + | x | - b Q b p = 0 , together with scaling condition | x | | ∇ g ( x ) | ≲ | x | - b , variational condition g s 2 p - 1 ( p + 1 2 - g i ) ≤ p - 1 2 , and rigidity condition - b g ( x ) ≤ x · ∇ g ( x ) . We also provide sharp finite time blow-up results for non-radial and radial solutions. For this, we utilize the localized virial identity.
ISSN:1424-3199
1424-3202
DOI:10.1007/s00028-020-00558-1