Strong ill-posedness and non-existence in Sobolev spaces for generalized-SQG
The general surface quasi-geostrophic equation is the scalar transport equation defined by { ∂ θ ∂ t + v 1 γ ∂ θ ∂ x 1 + v 2 γ ∂ θ ∂ x 2 = 0 , v γ = ∇ ⊥ ψ γ = ( ∂ 2 ψ γ , − ∂ 1 ψ γ ) , ψ γ = − Λ − 1 + γ θ , θ ( ⋅ , 0 ) = θ 0 ( ⋅ ) , for γ ∈ ( − 1 , 1 ) , where the non-local operator Λ α = ( − Δ ) α...
| Autores: | , , |
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| Tipo de recurso: | artículo |
| Estado: | Versión publicada |
| Fecha de publicación: | 2025 |
| País: | España |
| Institución: | Consejo Superior de Investigaciones Científicas (CSIC) |
| Repositorio: | DIGITAL.CSIC. Repositorio Institucional del CSIC |
| OAI Identifier: | oai:digital.csic.es:10261/425188 |
| Acceso en línea: | http://hdl.handle.net/10261/425188 https://www.scopus.com/inward/record.uri?eid=2-s2.0-105014192955&doi=10.1088%2F1361-6544%2Fadf9b1&partnerID=40&md5=820792b14a56ad9f340b67074585d518 |
| Access Level: | acceso abierto |
| Palabra clave: | non-existence strong ill-posedness surface quasi-geostrophic equation (SQG) |
| Sumario: | The general surface quasi-geostrophic equation is the scalar transport equation defined by { ∂ θ ∂ t + v 1 γ ∂ θ ∂ x 1 + v 2 γ ∂ θ ∂ x 2 = 0 , v γ = ∇ ⊥ ψ γ = ( ∂ 2 ψ γ , − ∂ 1 ψ γ ) , ψ γ = − Λ − 1 + γ θ , θ ( ⋅ , 0 ) = θ 0 ( ⋅ ) , for γ ∈ ( − 1 , 1 ) , where the non-local operator Λ α = ( − Δ ) α 2 is defined on the Fourier side by Λ α f ^ ( ξ ) = | ξ | α f ^ ( ξ ) . The PDE is well-posed in the Sobolev spaces Hs with s > 2 + γ . In this paper we prove strong ill-posedness in the super-critical regime Hβ with β ∈ [ 1 , 2 + γ ) ∩ ( 3 2 + γ , 2 + γ ) . To do this, we will derive an approximated PDE solvable by some family of functions that we will call pseudosolutions and that will allow us to control the norms of the real solutions. Using this result and a gluing argument we also prove non-existence of solutions in the same Sobolev spaces. Since the pseudosolution will control the real one, we can build a solution that will be initially in Hβ and will leave it instantaneously. Nevertheless, this solution exists for a long time and remains the only classical solution in a high regularity class. © 2025 The Author(s). Published by IOP Publishing Ltd and the London Mathematical Society. |
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