2024/09/07 by Zhao, Jason
Mathematics · #Advanced Mathematical Physics Problems #Analysis of PDEs (math.AP) #FOS: Mathematics
paper · pdf · doi:10.48550/arxiv.2409.04706
openalex publication_date 2024/09/07 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
Given sufficiently regular data without decay assumptions at infinity, we prove local well-posedness for non-linear dispersive equations of the form ∂t u + \mathsf A(∇) u + \mathcal Q(|u|2) ⋅ ∇ u= \mathcal N (u, u), where \mathsf A(∇) is a Fourier multiplier with purely imaginary symbol of order σ+ 1 for σ> 0, and polynomial-type non-linearities \mathcal Q(|u|2) and \mathcal N(u, u). Our approach revisits the classical energy method by applying it within a class of local Sobolev-type spaces ℓ^∞\mathsf A(ξ) Hs (\mathbb Rd) which are adapted to the dispersion relation in the sense that functions u localised to dyadic frequency |ξ| ≈ N have size ||u||_ℓ^∞\mathsf A(ξ) Hs ≈ Ns sup_diam(Q) = Nσ ||u||L2x (Q). In analogy with the classical Hs-theory, we prove ℓ^∞\mathsf A(ξ) Hs-local well-posedness for s > \tfracd2 + 1 for the derivative non-linear equation, and s > \tfracd2 without the derivative non-linearity. As an application, we show that if in addition the initial data is spatially almost periodic, then the solution is also spatially almost periodic.