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Strong illposedness for SQG in critical Sobolev spaces

In-Jee Jeong, Junha Kim

Abstract

We prove that the inviscid surface quasi-geostrophic (SQG) equations are strongly ill-posed in critical Sobolev spaces: there exists an initial data $H^{2}(\bbT^2)$ without any solutions in $L^\infty_{t}H^{2}$. Moreover, we prove strong critical norm inflation for $C^\infty$--smooth data. Our proof is robust and extends to give similar ill-posedness results for the family of modified SQG equations which interpolate the SQG with two-dimensional incompressible Euler equations.

Strong illposedness for SQG in critical Sobolev spaces

Abstract

We prove that the inviscid surface quasi-geostrophic (SQG) equations are strongly ill-posed in critical Sobolev spaces: there exists an initial data without any solutions in . Moreover, we prove strong critical norm inflation for --smooth data. Our proof is robust and extends to give similar ill-posedness results for the family of modified SQG equations which interpolate the SQG with two-dimensional incompressible Euler equations.

Paper Structure

This paper contains 12 sections, 8 theorems, 224 equations.

Key Result

Theorem A

For any $\epsilon, \delta, A> 0$, there exists $\theta_{0} \in C^\infty(\mathbb T^2)$ satisfying $\Vert\theta_0\Vert_{H^2 \cap W^{1,\infty}} < \epsilon$ such that the unique local-in-time smooth solution $\theta$ to eq:SQG with initial data $\theta_{0}$ exists on $[0,\delta^*]$ for some $0<\delta^*

Theorems & Definitions (18)

  • Theorem A: Strong norm inflation
  • Theorem B: Nonexistence
  • Remark 1.1
  • Lemma 3.1: Hardy's inequality
  • proof
  • Lemma 3.2
  • Remark 3.3
  • proof
  • Lemma 3.4
  • proof
  • ...and 8 more