<p>This paper is devoted to the Cauchy problem of the parabolic-parabolic Keller-Segel system with growth source and nonlinear secretion in any dimensional setting: <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1134_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="371" /> </InlineMediaObject> <EquationSource Format="TEX">\(u_t=\Delta u-\chi \nabla \cdot (u\nabla v )+f(u),v_t=\Delta v-\lambda v+g(u)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>-</mo> <mi>χ</mi> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mi mathvariant="normal">∇</mi> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <msub> <mi>v</mi> <mi>t</mi> </msub> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>v</mi> <mo>-</mo> <mi>λ</mi> <mi>v</mi> <mo>+</mo> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1134_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\chi ,\lambda &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>χ</mi> <mo>,</mo> <mi>λ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. The generalized logistic source <i>f</i>(<i>u</i>) satisfies <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1134_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="178" /> </InlineMediaObject> <EquationSource Format="TEX">\(0\le f(u)\le u(a-bu^{\gamma -1})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>≤</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>≤</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>a</mi> <mo>-</mo> <mi>b</mi> <msup> <mi>u</mi> <mrow> <mi>γ</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with some <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1134_Article_IEq4.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(a,b&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>,</mo> <mi>b</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1134_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma &gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>γ</mi> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>; the signal production term <i>g</i>(<i>u</i>) satisfies <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1134_Article_IEq6.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="114" /> </InlineMediaObject> <EquationSource Format="TEX">\(0\le g(u)\le \mu u^{k}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>≤</mo> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>≤</mo> <mi>μ</mi> <msup> <mi>u</mi> <mi>k</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1134_Article_IEq7.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu ,k&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>,</mo> <mi>k</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. We discuss the global boundedness of classical solutions with nonnegative bounded and uniformly continuous initial functions. Moreover, the solutions converging to positive constant equilibria is demonstrated for strictly positive initial data, building upon the persistence of classical solutions in the case of <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1134_Article_IEq8.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="221" /> </InlineMediaObject> <EquationSource Format="TEX">\(f(u)=u(a-bu^{\gamma -1}),\gamma \in (1,2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>a</mi> <mo>-</mo> <mi>b</mi> <msup> <mi>u</mi> <mrow> <mi>γ</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mi>γ</mi> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1134_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\(g(u)=\mu u\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>g</mi> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mi>μ</mi> <mi>u</mi> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Global boundedness and asymptotic stability of the Keller-Segel system with growth source in the whole space

  • Qingchun Li,
  • Haomeng Chen

摘要

This paper is devoted to the Cauchy problem of the parabolic-parabolic Keller-Segel system with growth source and nonlinear secretion in any dimensional setting: \(u_t=\Delta u-\chi \nabla \cdot (u\nabla v )+f(u),v_t=\Delta v-\lambda v+g(u)\) u t = Δ u - χ · ( u v ) + f ( u ) , v t = Δ v - λ v + g ( u ) , where \(\chi ,\lambda >0\) χ , λ > 0 . The generalized logistic source f(u) satisfies \(0\le f(u)\le u(a-bu^{\gamma -1})\) 0 f ( u ) u ( a - b u γ - 1 ) with some \(a,b>0\) a , b > 0 and \(\gamma >1\) γ > 1 ; the signal production term g(u) satisfies \(0\le g(u)\le \mu u^{k}\) 0 g ( u ) μ u k with \(\mu ,k>0\) μ , k > 0 . We discuss the global boundedness of classical solutions with nonnegative bounded and uniformly continuous initial functions. Moreover, the solutions converging to positive constant equilibria is demonstrated for strictly positive initial data, building upon the persistence of classical solutions in the case of \(f(u)=u(a-bu^{\gamma -1}),\gamma \in (1,2)\) f ( u ) = u ( a - b u γ - 1 ) , γ ( 1 , 2 ) and \(g(u)=\mu u\) g ( u ) = μ u .