<p>We consider the Cauchy problem for the logarithmically singular surface quasi-geostrophic (SQG) equation, introduced by Ohkitani, <Equation ID="Equ39"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5257_Article_Equ39.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="265" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \begin{aligned} \partial _t \theta - \nabla ^\perp \log (10+(-\Delta )^{\frac{1}{2}})\theta \cdot \nabla \theta = 0, \end{aligned} \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mi>θ</mi> <mo>-</mo> <msup> <mi mathvariant="normal">∇</mi> <mo>⊥</mo> </msup> <mo>log</mo> <mrow> <mo stretchy="false">(</mo> <mn>10</mn> <mo>+</mo> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </msup> <mo stretchy="false">)</mo> </mrow> <mi>θ</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>θ</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>and establish local existence and uniqueness of smooth solutions in the scale of Sobolev spaces with exponent decreasing with time. Such a decrease of the Sobolev exponent is necessary, as we have shown in the companion paper (Chae et al. in Illposedness via degenerate dispersion for generalized surface quasi-geostrophic equations with singular velocities, <a href="http://arxiv.org/abs/2308.02120">arXiv:2308.02120</a>) that the problem is strongly ill-posed in any fixed Sobolev spaces. The time dependence of the Sobolev exponent can be removed when there is a dissipation term strictly stronger than log. These results improve wellposedness statements by Chae et al. (Comm Pure Appl Math 65(8):1037–1066, 2012). This well-posedness result can be applied to describe the long-time dynamics of the <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5257_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\delta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>δ</mi> </math></EquationSource> </InlineEquation>-SQG equations, defined by <Equation ID="Equ40"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5257_Article_Equ40.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="256" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \begin{aligned} \partial _t \theta + \nabla ^\perp (10+(-\Delta )^{\frac{1}{2}})^{-\delta }\theta \cdot \nabla \theta = 0, \end{aligned} \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mi>θ</mi> <mo>+</mo> <msup> <mi mathvariant="normal">∇</mi> <mo>⊥</mo> </msup> <msup> <mrow> <mo stretchy="false">(</mo> <mn>10</mn> <mo>+</mo> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </msup> <mo stretchy="false">)</mo> </mrow> <mrow> <mo>-</mo> <mi>δ</mi> </mrow> </msup> <mi>θ</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>θ</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>for all sufficiently small <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5257_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(\delta &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>δ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> depending on the size of the initial data. For the same range of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5257_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\delta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>δ</mi> </math></EquationSource> </InlineEquation>, we establish global well-posedness of smooth solutions to the dissipative SQG equations.</p>

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Well-Posedness for Ohkitani Model and Long-Time Existence for Surface Quasi-geostrophic Equations

  • Dongho Chae,
  • In-Jee Jeong,
  • Jungkyoung Na,
  • Sung-Jin Oh

摘要

We consider the Cauchy problem for the logarithmically singular surface quasi-geostrophic (SQG) equation, introduced by Ohkitani, \(\begin{aligned} \begin{aligned} \partial _t \theta - \nabla ^\perp \log (10+(-\Delta )^{\frac{1}{2}})\theta \cdot \nabla \theta = 0, \end{aligned} \end{aligned}\) t θ - log ( 10 + ( - Δ ) 1 2 ) θ · θ = 0 , and establish local existence and uniqueness of smooth solutions in the scale of Sobolev spaces with exponent decreasing with time. Such a decrease of the Sobolev exponent is necessary, as we have shown in the companion paper (Chae et al. in Illposedness via degenerate dispersion for generalized surface quasi-geostrophic equations with singular velocities, arXiv:2308.02120) that the problem is strongly ill-posed in any fixed Sobolev spaces. The time dependence of the Sobolev exponent can be removed when there is a dissipation term strictly stronger than log. These results improve wellposedness statements by Chae et al. (Comm Pure Appl Math 65(8):1037–1066, 2012). This well-posedness result can be applied to describe the long-time dynamics of the \(\delta \) δ -SQG equations, defined by \(\begin{aligned} \begin{aligned} \partial _t \theta + \nabla ^\perp (10+(-\Delta )^{\frac{1}{2}})^{-\delta }\theta \cdot \nabla \theta = 0, \end{aligned} \end{aligned}\) t θ + ( 10 + ( - Δ ) 1 2 ) - δ θ · θ = 0 , for all sufficiently small \(\delta >0\) δ > 0 depending on the size of the initial data. For the same range of \(\delta \) δ , we establish global well-posedness of smooth solutions to the dissipative SQG equations.