<p>We establish the existence of positive self-similar solutions for the nonlinear homogeneous parabolic system given by <Equation ID="Equ150"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} u_t-\Delta u=\mu _1|u|^{2p}u+\beta |v|^{p+1}|u|^{p-1} u\ \ {\text {in}}\ \ (0,\infty )\times \mathbb {R}^N,\\ v_t-\Delta v=\mu _2|v|^{2p}v+\beta |u|^{p+1}|v|^{p-1} v\ \ {\text {in}}\ \ (0,\infty )\times \mathbb {R}^N,\\ u(0,x)=u_0(x),\ \ v(0,x)=v_0(x) \ \ {\text {in}}\ \ \mathbb {R}^N, \end{array}\right. } \end{aligned}\)</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> <mi>u</mi> <mo>=</mo> <msub> <mi>μ</mi> <mn>1</mn> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mn>2</mn> <mi>p</mi> </mrow> </msup> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mi>β</mi> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi>u</mi> <mspace width="4pt" /> <mspace width="4pt" /> <mtext>in</mtext> <mspace width="4pt" /> <mspace width="4pt" /> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <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> <mi>v</mi> <mo>=</mo> <msub> <mi>μ</mi> <mn>2</mn> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mn>2</mn> <mi>p</mi> </mrow> </msup> <mi>v</mi> <mo>+</mo> <msup> <mrow> <mi>β</mi> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi>v</mi> <mspace width="4pt" /> <mspace width="4pt" /> <mtext>in</mtext> <mspace width="4pt" /> <mspace width="4pt" /> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi>u</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="4pt" /> <mspace width="4pt" /> <mi>v</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi>v</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="4pt" /> <mspace width="4pt" /> <mtext>in</mtext> <mspace width="4pt" /> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(N=3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(1&lt;p&lt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mu _1,\mu _2,\beta &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>μ</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>μ</mi> <mn>2</mn> </msub> <mo>,</mo> <mi>β</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(u_0(x), v_0(x)\ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>u</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <msub> <mi>v</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Our approach involves demonstrating the existence of positive self-similar solutions with appropriate initial values. Additionally, we construct perturbations of the positive self-similar solution with more general initial values using a contraction mapping argument. Compared to previous works, we encounter new challenges due to the utilization of shooting methods. Fortunately, these challenges can be overcome by carefully studying the properties of the self-similar solutions.</p>

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Existence and multiplicity of positive solutions for the parabolic system with singular data

  • Qiuping Geng,
  • Jun Wang

摘要

We establish the existence of positive self-similar solutions for the nonlinear homogeneous parabolic system given by \(\begin{aligned} {\left\{ \begin{array}{ll} u_t-\Delta u=\mu _1|u|^{2p}u+\beta |v|^{p+1}|u|^{p-1} u\ \ {\text {in}}\ \ (0,\infty )\times \mathbb {R}^N,\\ v_t-\Delta v=\mu _2|v|^{2p}v+\beta |u|^{p+1}|v|^{p-1} v\ \ {\text {in}}\ \ (0,\infty )\times \mathbb {R}^N,\\ u(0,x)=u_0(x),\ \ v(0,x)=v_0(x) \ \ {\text {in}}\ \ \mathbb {R}^N, \end{array}\right. } \end{aligned}\) u t - Δ u = μ 1 | u | 2 p u + β | v | p + 1 | u | p - 1 u in ( 0 , ) × R N , v t - Δ v = μ 2 | v | 2 p v + β | u | p + 1 | v | p - 1 v in ( 0 , ) × R N , u ( 0 , x ) = u 0 ( x ) , v ( 0 , x ) = v 0 ( x ) in R N , where \(N=3\) N = 3 , \(1<p<2\) 1 < p < 2 , \(\mu _1,\mu _2,\beta >0\) μ 1 , μ 2 , β > 0 , and \(u_0(x), v_0(x)\ge 0\) u 0 ( x ) , v 0 ( x ) 0 . Our approach involves demonstrating the existence of positive self-similar solutions with appropriate initial values. Additionally, we construct perturbations of the positive self-similar solution with more general initial values using a contraction mapping argument. Compared to previous works, we encounter new challenges due to the utilization of shooting methods. Fortunately, these challenges can be overcome by carefully studying the properties of the self-similar solutions.