<p>The behavior of positive solutions of the nonlocal elliptic problem <Equation ID="Equ75"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} \Delta u+\lambda u-[a(x)+\varepsilon ]u^p-b(x)u\int _\Omega c(y)u^r(y)\,dy=0,&amp; x\in \Omega ,\\ u=0,&amp; x\in \partial \Omega , \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <mi>u</mi> <mo>-</mo> <mrow> <mo stretchy="false">[</mo> <mi>a</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>ε</mi> <mo stretchy="false">]</mo> </mrow> <msup> <mi>u</mi> <mi>p</mi> </msup> <mo>-</mo> <mi>b</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <mi>c</mi> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mi>u</mi> <mi>r</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="0.166667em" /> <mi>d</mi> <mi>y</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>is studied, where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega \subset {\mathbb {R}}^N (N\ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi>N</mi> <mo>≥</mo> <mn>1</mn> </mrow> </mrow> </math></EquationSource> </InlineEquation>) is a bounded domain with smooth boundary, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\lambda &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(p&gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(r\ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>r</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, <i>a</i>, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(b\in C^\alpha (\bar{\Omega })\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>b</mi> <mo>∈</mo> <msup> <mi>C</mi> <mi>α</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mover accent="true"> <mrow> <mi mathvariant="normal">Ω</mi> </mrow> <mrow> <mo stretchy="false">¯</mo> </mrow> </mover> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(0&lt;\alpha &lt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>α</mi> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> are nonnegative functions, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(c\in L^\infty (\Omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>∈</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> satisfies <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(c&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\varepsilon &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is a small perturbation parameter. It is known for the case <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\varepsilon =0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> that spatial degeneracies in the functions <i>a</i> and <i>b</i> can fundamentally change the structure of positive solutions. In order to find the essential role of spatial degeneracies, we examine the asymptotic profiles as <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\varepsilon \rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and show that the degeneracy of <i>a</i> and <i>b</i> induces sharp patterns of positive solutions in the region where both coefficients <i>a</i> and <i>b</i> exhibit degeneracies. In sharp contrast to classical reaction-diffusion equations, the presence of the nonlocal term causes the positive solution to decay to zero as <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\varepsilon \rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> in the region where <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(b&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>b</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Asymptotic profiles of positive solutions in a nonlocal elliptic problem

  • Jian-Wen Sun,
  • Christoph Walker,
  • Yan-Hua Xing

摘要

The behavior of positive solutions of the nonlocal elliptic problem \(\begin{aligned} {\left\{ \begin{array}{ll} \Delta u+\lambda u-[a(x)+\varepsilon ]u^p-b(x)u\int _\Omega c(y)u^r(y)\,dy=0,& x\in \Omega ,\\ u=0,& x\in \partial \Omega , \end{array}\right. } \end{aligned}\) Δ u + λ u - [ a ( x ) + ε ] u p - b ( x ) u Ω c ( y ) u r ( y ) d y = 0 , x Ω , u = 0 , x Ω , is studied, where \(\Omega \subset {\mathbb {R}}^N (N\ge 1\) Ω R N ( N 1 ) is a bounded domain with smooth boundary, \(\lambda >0\) λ > 0 , \(p>1\) p > 1 and \(r\ge 1\) r 1 , a, \(b\in C^\alpha (\bar{\Omega })\) b C α ( Ω ¯ ) with \(0<\alpha <1\) 0 < α < 1 are nonnegative functions, \(c\in L^\infty (\Omega )\) c L ( Ω ) satisfies \(c>0\) c > 0 , and \(\varepsilon >0\) ε > 0 is a small perturbation parameter. It is known for the case \(\varepsilon =0\) ε = 0 that spatial degeneracies in the functions a and b can fundamentally change the structure of positive solutions. In order to find the essential role of spatial degeneracies, we examine the asymptotic profiles as \(\varepsilon \rightarrow 0\) ε 0 and show that the degeneracy of a and b induces sharp patterns of positive solutions in the region where both coefficients a and b exhibit degeneracies. In sharp contrast to classical reaction-diffusion equations, the presence of the nonlocal term causes the positive solution to decay to zero as \(\varepsilon \rightarrow 0\) ε 0 in the region where \(b>0\) b > 0 .