<p>In this work, we consider the initial value problem (IVP) for a system of modified Korteweg-de Vries (mKdV) equations <Equation ID="Equa"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_Equa.gif" Format="GIF" Height="43" Rendition="HTML" Resolution="72" Type="Linedraw" Width="341" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} \partial _t v + \partial _x^3 v+ \partial _x (v w^2) = 0, \hspace{0.98 cm} v(x,0)=\psi (x),\\ \partial _t w + \alpha \partial _x^3 w+\partial _x (v^2 w) = 0,\hspace{0.5 cm} w(x,0)=\phi (x). \end{array}\right. } \end{aligned}\)</EquationSource> </Equation>The main interest is in addressing the well-posedness issues of the IVP when the initial data are considered in the modulation space <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(M_s^{2,p}(\mathbb R)\)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\ge 2\)</EquationSource> </InlineEquation>. In the case when <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="73" /> </InlineMediaObject> <EquationSource Format="TEX">\(0&lt;\alpha \ne 1\)</EquationSource> </InlineEquation>, we derive new trilinear estimates in these spaces and prove that the IVP is locally well-posed for data in <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(M_s^{2,p}(\mathbb R)\)</EquationSource> </InlineEquation> whenever <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq5.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="70" /> </InlineMediaObject> <EquationSource Format="TEX">\(s&gt; \frac{1}{4}-\frac{1}{p}\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\ge 2\)</EquationSource> </InlineEquation>. In deriving the trilinear estimate, the fact that the Fourier supports of the solution components <i>v</i> and <i>w</i> lie on distinct cubic curves, namely <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tau = \xi ^3\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tau = \alpha \xi ^3\)</EquationSource> </InlineEquation>, introduces additional difficulties in handling the resonant case. This makes the analysis substantially different from what one encounters in the single-equation setting. To overcome the difficulties arising in the resonant case, it was necessary to impose the more restrictive condition <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq5.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="70" /> </InlineMediaObject> <EquationSource Format="TEX">\(s&gt; \frac{1}{4}-\frac{1}{p}\)</EquationSource> </InlineEquation> on the trilinear estimate, rather than the natural threshold <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq10.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="76" /> </InlineMediaObject> <EquationSource Format="TEX">\(s&gt; \frac{1}{4}-\frac{3}{2p}\)</EquationSource> </InlineEquation> , which would otherwise yield sharp local well-posedness for <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq11.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="TEX">\(s&gt;-\frac{1}{2}\)</EquationSource> </InlineEquation> when <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12591_2025_741_Article_IEq12.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(p=2\)</EquationSource> </InlineEquation>.</p>

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Local Well-Posedness for a System of Modified KdV Equations in Modulation Spaces

  • X. Carvajal,
  • F. Cuba,
  • M. Panthee

摘要

In this work, we consider the initial value problem (IVP) for a system of modified Korteweg-de Vries (mKdV) equations \(\begin{aligned} {\left\{ \begin{array}{ll} \partial _t v + \partial _x^3 v+ \partial _x (v w^2) = 0, \hspace{0.98 cm} v(x,0)=\psi (x),\\ \partial _t w + \alpha \partial _x^3 w+\partial _x (v^2 w) = 0,\hspace{0.5 cm} w(x,0)=\phi (x). \end{array}\right. } \end{aligned}\) The main interest is in addressing the well-posedness issues of the IVP when the initial data are considered in the modulation space \(M_s^{2,p}(\mathbb R)\) , \(p\ge 2\) . In the case when \(0<\alpha \ne 1\) , we derive new trilinear estimates in these spaces and prove that the IVP is locally well-posed for data in \(M_s^{2,p}(\mathbb R)\) whenever \(s> \frac{1}{4}-\frac{1}{p}\) and \(p\ge 2\) . In deriving the trilinear estimate, the fact that the Fourier supports of the solution components v and w lie on distinct cubic curves, namely \(\tau = \xi ^3\) and \(\tau = \alpha \xi ^3\) , introduces additional difficulties in handling the resonant case. This makes the analysis substantially different from what one encounters in the single-equation setting. To overcome the difficulties arising in the resonant case, it was necessary to impose the more restrictive condition \(s> \frac{1}{4}-\frac{1}{p}\) on the trilinear estimate, rather than the natural threshold \(s> \frac{1}{4}-\frac{3}{2p}\) , which would otherwise yield sharp local well-posedness for \(s>-\frac{1}{2}\) when \(p=2\) .