<p>In this paper, we investigate a Stokes-Magneto system with fractional diffusions. We first deal with the non-resistive case in <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42985_2025_341_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {T}}^{d}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">T</mi> </mrow> <mi>d</mi> </msup> </math></EquationSource> </InlineEquation> and establish the local and global well-posedness with initial magnetic field <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42985_2025_341_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="93" /> </InlineMediaObject> <EquationSource Format="TEX">\({\varvec{b}}_0\in H^{s}({\mathbb {T}}^d).\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi mathvariant="bold-italic">b</mi> </mrow> <mn>0</mn> </msub> <mo>∈</mo> <msup> <mi>H</mi> <mi>s</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">T</mi> </mrow> <mi>d</mi> </msup> <mo stretchy="false">)</mo> </mrow> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> We also show the existence of a unique mild solution of the resistive case with initial data <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42985_2025_341_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\({\varvec{b}}_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mi mathvariant="bold-italic">b</mi> </mrow> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> in the critical <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42985_2025_341_Article_IEq4.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^{p}({\mathbb {R}}^d)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> space. Moreover, we show that <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42985_2025_341_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Vert {\varvec{b}}(t)\Vert _{L^{p}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">‖</mo> <mrow> <mi mathvariant="bold-italic">b</mi> </mrow> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">‖</mo> </mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> </msub> </math></EquationSource> </InlineEquation> converges to zero as <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42985_2025_341_Article_IEq6.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(t\rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> when the initial data is sufficiently small.</p>

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Local and global solutions to Stokes-Magneto equations with fractional dissipations

  • Hantaek Bae,
  • Hyunwoo Kwon,
  • Jaeyong Shin

摘要

In this paper, we investigate a Stokes-Magneto system with fractional diffusions. We first deal with the non-resistive case in \({\mathbb {T}}^{d}\) T d and establish the local and global well-posedness with initial magnetic field \({\varvec{b}}_0\in H^{s}({\mathbb {T}}^d).\) b 0 H s ( T d ) . We also show the existence of a unique mild solution of the resistive case with initial data \({\varvec{b}}_0\) b 0 in the critical \(L^{p}({\mathbb {R}}^d)\) L p ( R d ) space. Moreover, we show that \(\Vert {\varvec{b}}(t)\Vert _{L^{p}}\) b ( t ) L p converges to zero as \(t\rightarrow \infty \) t when the initial data is sufficiently small.