<p>In this paper, we consider the qualitative analysis for a general form of <i>n</i>-dimension Keller–Segel system with logistic sources (include the parabolic-elliptic Keller–Segel (PEKS) system and the corresponding hyperbolic-elliptic Keller–Segel (HEKS) system). By the transport (-diffusion) theory, we first establish the local existence and uniqueness of strong solutions to (PEKS) and (HEKS) for the initial data in <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq1.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(B_{p,r}^{s}({\mathbb {R}}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>B</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> </mrow> <mi>s</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq2.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="107" /> </InlineMediaObject> <EquationSource Format="TEX">\(s&gt; \max \{\frac{n}{p},\frac{1}{2}\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>&gt;</mo> <mo movablelimits="true">max</mo> <mo stretchy="false">{</mo> <mfrac> <mi>n</mi> <mi>p</mi> </mfrac> <mo>,</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mo stretchy="false">}</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="99" /> </InlineMediaObject> <EquationSource Format="TEX">\(1\le p,r \le \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>≤</mo> <mi>p</mi> <mo>,</mo> <mi>r</mi> <mo>≤</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> (or <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq4.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(s=\frac{n}{p}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>=</mo> <mfrac> <mi>n</mi> <mi>p</mi> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="127" /> </InlineMediaObject> <EquationSource Format="TEX">\(1\le p\le 2n, r=1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>≤</mo> <mi>p</mi> <mo>≤</mo> <mn>2</mn> <mi>n</mi> <mo>,</mo> <mi>r</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>) and also obtain the continuity of the solution map with respect to the initial data in the space <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq6.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="284" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {C}}([0;T];B^{s'}_{p,r}({\mathbb {R}}^n))\cap {\mathcal {C}}^1([0;T];B^{s'-1}_{p,r}({\mathbb {R}}^n))\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">C</mi> <mrow> <mo stretchy="false">(</mo> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>;</mo> <mi>T</mi> <mo stretchy="false">]</mo> </mrow> <mo>;</mo> <msubsup> <mi>B</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> </mrow> <msup> <mi>s</mi> <mo>′</mo> </msup> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo>∩</mo> <msup> <mrow> <mi mathvariant="script">C</mi> </mrow> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>;</mo> <mi>T</mi> <mo stretchy="false">]</mo> </mrow> <mo>;</mo> <msubsup> <mi>B</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> </mrow> <mrow> <msup> <mi>s</mi> <mo>′</mo> </msup> <mo>-</mo> <mn>1</mn> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for every <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq7.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(s'&lt;s\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>s</mi> <mo>′</mo> </msup> <mo>&lt;</mo> <mi>s</mi> </mrow> </math></EquationSource> </InlineEquation> when <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq8.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="63" /> </InlineMediaObject> <EquationSource Format="TEX">\(r=+\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>r</mi> <mo>=</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq9.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\(s'=s\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>s</mi> <mo>′</mo> </msup> <mo>=</mo> <mi>s</mi> </mrow> </math></EquationSource> </InlineEquation> when <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq10.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="TEX">\(r&lt;+\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>r</mi> <mo>&lt;</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> and then derive a continuation criterion result for (HEKS). In addition, we prove that this data-to-solution map for (PEKS) is discontinuous in the metric of <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq11.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="37" /> </InlineMediaObject> <EquationSource Format="TEX">\(B_{2,\infty }^s\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>B</mi> <mrow> <mn>2</mn> <mo>,</mo> <mi>∞</mi> </mrow> <mi>s</mi> </msubsup> </math></EquationSource> </InlineEquation>. Furthermore, we show that the inviscid limit of the (PEKS) converges to the (HEKS) in the same topology of Besov spaces as the initial data <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2442_Article_IEq12.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="97" /> </InlineMediaObject> <EquationSource Format="TEX">\(u_0\in B_{p,r}^s({\mathbb {R}}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>u</mi> <mn>0</mn> </msub> <mo>∈</mo> <msubsup> <mi>B</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> </mrow> <mi>s</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>.</p>

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The local well-posedness and inviscid limit for a general form of Keller–Segel equation with logistic sources

  • Shanshan Zheng,
  • Shouming Zhou,
  • Li Yang

摘要

In this paper, we consider the qualitative analysis for a general form of n-dimension Keller–Segel system with logistic sources (include the parabolic-elliptic Keller–Segel (PEKS) system and the corresponding hyperbolic-elliptic Keller–Segel (HEKS) system). By the transport (-diffusion) theory, we first establish the local existence and uniqueness of strong solutions to (PEKS) and (HEKS) for the initial data in \(B_{p,r}^{s}({\mathbb {R}}^n)\) B p , r s ( R n ) with \(s> \max \{\frac{n}{p},\frac{1}{2}\}\) s > max { n p , 1 2 } , \(1\le p,r \le \infty \) 1 p , r (or \(s=\frac{n}{p}\) s = n p , \(1\le p\le 2n, r=1\) 1 p 2 n , r = 1 ) and also obtain the continuity of the solution map with respect to the initial data in the space \({\mathcal {C}}([0;T];B^{s'}_{p,r}({\mathbb {R}}^n))\cap {\mathcal {C}}^1([0;T];B^{s'-1}_{p,r}({\mathbb {R}}^n))\) C ( [ 0 ; T ] ; B p , r s ( R n ) ) C 1 ( [ 0 ; T ] ; B p , r s - 1 ( R n ) ) for every \(s'<s\) s < s when \(r=+\infty \) r = + or \(s'=s\) s = s when \(r<+\infty \) r < + and then derive a continuation criterion result for (HEKS). In addition, we prove that this data-to-solution map for (PEKS) is discontinuous in the metric of \(B_{2,\infty }^s\) B 2 , s . Furthermore, we show that the inviscid limit of the (PEKS) converges to the (HEKS) in the same topology of Besov spaces as the initial data \(u_0\in B_{p,r}^s({\mathbb {R}}^n)\) u 0 B p , r s ( R n ) .