A Conjecture Regarding Optimal Strichartz Estimates for the Wave Equation

Author(s):  
Neal Bez ◽  
Chris Jeavons ◽  
Tohru Ozawa ◽  
Hiroki Saito
2021 ◽  
Vol 300 ◽  
pp. 830-880
Author(s):  
Oana Ivanovici ◽  
Gilles Lebeau ◽  
Fabrice Planchon

2021 ◽  
Vol 273 (1339) ◽  
Author(s):  
Gong Chen

We prove Strichartz estimates (both regular and reversed) for a scattering state to the wave equation with a charge transfer Hamiltonian in R 3 \mathbb {R}^{3} : \[ ∂ t t u − Δ u + ∑ j = 1 m V j ( x − v → j t ) u = 0. \partial _{tt}u-\Delta u+\sum _{j=1}^{m}V_{j}\left (x-\vec {v}_{j}t\right )u=0. \] The energy estimate and the local energy decay of a scattering state are also established. In order to study nonlinear multisoltion systems, we will present the inhomogeneous generalizations of Strichartz estimates and local decay estimates. As an application of our results, we show that scattering states indeed scatter to solutions to the free wave equation. These estimates for this linear models are also of crucial importance for problems related to interactions of potentials and solitons, for example, in [Comm. Math. Phys. 364 (2018), no. 1, pp. 45–82].


2014 ◽  
Vol 11 (03) ◽  
pp. 437-476 ◽  
Author(s):  
Marius Beceanu

Consider the focusing semilinear wave equation in ℝ3 with energy-critical nonlinearity [Formula: see text] This equation admits stationary solutions of the form [Formula: see text] called solitons, which solve the elliptic equation [Formula: see text] Restricting ourselves to the space of symmetric solutions ψ for which ψ(x) = ψ(-x), we find a local center-stable manifold, in a neighborhood of ϕ(x, 1), for this wave equation in the weighted Sobolev space [Formula: see text] Solutions with initial data on the manifold exist globally in time for t ≥ 0, depend continuously on initial data, preserve energy, and can be written as the sum of a rescaled soliton and a dispersive radiation term. The proof is based on a new class of reverse Strichartz estimates, recently introduced by Beceanu and Goldberg and adapted here to the case of Hamiltonians with a resonance.


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