<p>This paper deals with a two-species competition system with density-dependent motility and indirect signal production <Equation ID="Equ91"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="11587_2024_926_Article_Equ91.gif" Format="GIF" Height="95" Rendition="HTML" Resolution="72" Type="Linedraw" Width="412" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} u_t=\Delta \left( \gamma _1\left( w\right) u\right) +\mu _1u\left( 1-u-a_1v\right) ,\quad &amp; x\in \Omega ,\quad t&gt;0,\\ v_t=\Delta \left( \gamma _2\left( w\right) v\right) +\mu _2v\left( 1-v-a_2u\right) ,\quad &amp; x\in \Omega ,\quad t&gt;0,\\ w_t=\Delta w-w+z,\quad &amp; x\in \Omega ,\quad t&gt;0,\\ z_t=\Delta z-z+u+v,\quad &amp; x\in \Omega ,\quad t&gt;0, \end{array}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mfenced close=")" open="("> <msub> <mi>γ</mi> <mn>1</mn> </msub> <mfenced close=")" open="("> <mi>w</mi> </mfenced> <mi>u</mi> </mfenced> <mo>+</mo> <msub> <mi>μ</mi> <mn>1</mn> </msub> <mi>u</mi> <mfenced close=")" open="("> <mn>1</mn> <mo>-</mo> <mi>u</mi> <mo>-</mo> <msub> <mi>a</mi> <mn>1</mn> </msub> <mi>v</mi> </mfenced> <mo>,</mo> <mspace width="1em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="1em" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>v</mi> <mi>t</mi> </msub> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mfenced close=")" open="("> <msub> <mi>γ</mi> <mn>2</mn> </msub> <mfenced close=")" open="("> <mi>w</mi> </mfenced> <mi>v</mi> </mfenced> <mo>+</mo> <msub> <mi>μ</mi> <mn>2</mn> </msub> <mi>v</mi> <mfenced close=")" open="("> <mn>1</mn> <mo>-</mo> <mi>v</mi> <mo>-</mo> <msub> <mi>a</mi> <mn>2</mn> </msub> <mi>u</mi> </mfenced> <mo>,</mo> <mspace width="1em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="1em" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>w</mi> <mi>t</mi> </msub> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>w</mi> <mo>-</mo> <mi>w</mi> <mo>+</mo> <mi>z</mi> <mo>,</mo> <mspace width="1em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="1em" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>z</mi> <mi>t</mi> </msub> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>z</mi> <mo>-</mo> <mi>z</mi> <mo>+</mo> <mi>u</mi> <mo>+</mo> <mi>v</mi> <mo>,</mo> <mspace width="1em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="1em" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>under a smooth bounded domain <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11587_2024_926_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> with homogeneous Neumann boundary conditions. For <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11587_2024_926_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="TEX">\(i=1,2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, the parameters <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11587_2024_926_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu _{i}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mi>i</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11587_2024_926_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(a_{i}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>a</mi> <mi>i</mi> </msub> </math></EquationSource> </InlineEquation> are assumed to be positive. By some appropriate conditions on the density-dependent motility functions <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11587_2024_926_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma _{i}(w)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>γ</mi> <mi>i</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>w</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, we establish the global boundedness of the classical solutions of the system for any <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11587_2024_926_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu _{i}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mi>i</mi> </msub> </math></EquationSource> </InlineEquation>. Moreover, through the utilization of specific Lyapunov functionals, we establish the asymptotic stability of the solution under suitably chosen parameter conditions.</p>

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Boundedness and stabilization in a two-species competition system with density-dependent motility and indirect signal production

  • Lei Huang,
  • Fugeng Zeng,
  • Luxu Zhou,
  • Youjun Lu

摘要

This paper deals with a two-species competition system with density-dependent motility and indirect signal production \(\begin{aligned} \left\{ \begin{array}{ll} u_t=\Delta \left( \gamma _1\left( w\right) u\right) +\mu _1u\left( 1-u-a_1v\right) ,\quad & x\in \Omega ,\quad t>0,\\ v_t=\Delta \left( \gamma _2\left( w\right) v\right) +\mu _2v\left( 1-v-a_2u\right) ,\quad & x\in \Omega ,\quad t>0,\\ w_t=\Delta w-w+z,\quad & x\in \Omega ,\quad t>0,\\ z_t=\Delta z-z+u+v,\quad & x\in \Omega ,\quad t>0, \end{array}\right. \end{aligned}\) u t = Δ γ 1 w u + μ 1 u 1 - u - a 1 v , x Ω , t > 0 , v t = Δ γ 2 w v + μ 2 v 1 - v - a 2 u , x Ω , t > 0 , w t = Δ w - w + z , x Ω , t > 0 , z t = Δ z - z + u + v , x Ω , t > 0 , under a smooth bounded domain \(\Omega \subset \mathbb {R}^2\) Ω R 2 with homogeneous Neumann boundary conditions. For \(i=1,2\) i = 1 , 2 , the parameters \(\mu _{i}\) μ i and \(a_{i}\) a i are assumed to be positive. By some appropriate conditions on the density-dependent motility functions \(\gamma _{i}(w)\) γ i ( w ) , we establish the global boundedness of the classical solutions of the system for any \(\mu _{i}\) μ i . Moreover, through the utilization of specific Lyapunov functionals, we establish the asymptotic stability of the solution under suitably chosen parameter conditions.