<p>In this paper, we consider a coupled parabolic system with multiple Henón-type components <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\left( \partial _t \textbf{u} - \Delta _{\mathbb {G}} \textbf{u} \right) (x,t) = H(x,t,\textbf{u})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mfenced close=")" open="("> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mi mathvariant="bold">u</mi> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi mathvariant="double-struck">G</mi> </msub> <mi mathvariant="bold">u</mi> </mfenced> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi>H</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo>,</mo> <mi mathvariant="bold">u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\( (x,t) \in \mathbb {G} \times (0,T)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>∈</mo> <mi mathvariant="double-struck">G</mi> <mo>×</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\textbf{u}=(u_1,\cdots ,u_m) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold">u</mi> <mo>=</mo> <mo stretchy="false">(</mo> <msub> <mi>u</mi> <mn>1</mn> </msub> <mo>,</mo> <mo>⋯</mo> <mo>,</mo> <msub> <mi>u</mi> <mi>m</mi> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is the unknown, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathbb {G}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">G</mi> </math></EquationSource> </InlineEquation> is a homogeneous Carnot group on <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathbb {R}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\Delta _{\mathbb {G}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mi mathvariant="double-struck">G</mi> </msub> </math></EquationSource> </InlineEquation> is the operator whose components are given by the sub-Laplacian on <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathbb {G}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">G</mi> </math></EquationSource> </InlineEquation>, and <Equation ID="Equ54"> <EquationSource Format="TEX">\(\begin{aligned} H(x,t ,\textbf{u})=\left( t^{s_1} \ |x|_{\mathbb {G}}^{\gamma _1} \ u_2^{p_1}, t^{s_2} \ |x|_{\mathbb {G}}^{\gamma _2} \ u_3^{p_2}, \cdots , t^{s_{m}} \ |x|_{\mathbb {G}}^{\gamma _{m}} \ u_1^{p_{m}} \right) , \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi>H</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo>,</mo> <mi mathvariant="bold">u</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mfenced close=")" open="("> <msup> <mi>t</mi> <msub> <mi>s</mi> <mn>1</mn> </msub> </msup> <msubsup> <mrow> <mspace width="4pt" /> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi mathvariant="double-struck">G</mi> </mrow> <msub> <mi>γ</mi> <mn>1</mn> </msub> </msubsup> <mspace width="4pt" /> <msubsup> <mi>u</mi> <mn>2</mn> <msub> <mi>p</mi> <mn>1</mn> </msub> </msubsup> <mo>,</mo> <msup> <mi>t</mi> <msub> <mi>s</mi> <mn>2</mn> </msub> </msup> <msubsup> <mrow> <mspace width="4pt" /> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi mathvariant="double-struck">G</mi> </mrow> <msub> <mi>γ</mi> <mn>2</mn> </msub> </msubsup> <mspace width="4pt" /> <msubsup> <mi>u</mi> <mn>3</mn> <msub> <mi>p</mi> <mn>2</mn> </msub> </msubsup> <mo>,</mo> <mo>⋯</mo> <mo>,</mo> <msup> <mi>t</mi> <msub> <mi>s</mi> <mi>m</mi> </msub> </msup> <mspace width="4pt" /> <msubsup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi mathvariant="double-struck">G</mi> </mrow> <msub> <mi>γ</mi> <mi>m</mi> </msub> </msubsup> <mspace width="4pt" /> <msubsup> <mi>u</mi> <mn>1</mn> <msub> <mi>p</mi> <mi>m</mi> </msub> </msubsup> </mfenced> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>with <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(p_i \ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>p</mi> <mi>i</mi> </msub> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\textstyle \prod _{i=1}^m p_i&gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mstyle displaystyle="false" scriptlevel="0"> <mrow> <msubsup> <mo>∏</mo> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>m</mi> </msubsup> <msub> <mi>p</mi> <mi>i</mi> </msub> <mo>&gt;</mo> <mn>1</mn> </mrow> </mstyle> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\gamma _i\ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>γ</mi> <mi>i</mi> </msub> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(s_i&gt; -1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>s</mi> <mi>i</mi> </msub> <mo>&gt;</mo> <mo>-</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(i =1, \cdots , m\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mo>⋯</mo> <mo>,</mo> <mi>m</mi> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(|\cdot |_{\mathbb {G}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">|</mo> <mo>·</mo> <mo stretchy="false">|</mo> </mrow> <mi mathvariant="double-struck">G</mi> </msub> </math></EquationSource> </InlineEquation> denotes a homogeneous norm on <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\mathbb {G}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">G</mi> </math></EquationSource> </InlineEquation>. We determine the Fujita-type exponent for this system, which depends on the homogeneous dimension <i>Q</i> of <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\mathbb {G}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">G</mi> </math></EquationSource> </InlineEquation>. In contrast to previous studies, our results are obtained by iterative methods involving the symmetric submarkovian semigroup associated with the operator <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\Delta _{\mathbb {G}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mi mathvariant="double-struck">G</mi> </msub> </math></EquationSource> </InlineEquation>. In particular, the derivation of the blow-up result is delicate and is carried out through a novel approach based on Stirling’s asymptotic formula.</p>

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Fujita-Type Results for a Coupled Parabolic System of Hénon-Type Equations on Homogeneous Carnot Groups

  • Ricardo Freire,
  • Ricardo Castillo,
  • Miguel Loayza

摘要

In this paper, we consider a coupled parabolic system with multiple Henón-type components \(\left( \partial _t \textbf{u} - \Delta _{\mathbb {G}} \textbf{u} \right) (x,t) = H(x,t,\textbf{u})\) t u - Δ G u ( x , t ) = H ( x , t , u ) for \( (x,t) \in \mathbb {G} \times (0,T)\) ( x , t ) G × ( 0 , T ) , where \(\textbf{u}=(u_1,\cdots ,u_m) \) u = ( u 1 , , u m ) is the unknown, \(\mathbb {G}\) G is a homogeneous Carnot group on \(\mathbb {R}^N\) R N , \(\Delta _{\mathbb {G}}\) Δ G is the operator whose components are given by the sub-Laplacian on \(\mathbb {G}\) G , and \(\begin{aligned} H(x,t ,\textbf{u})=\left( t^{s_1} \ |x|_{\mathbb {G}}^{\gamma _1} \ u_2^{p_1}, t^{s_2} \ |x|_{\mathbb {G}}^{\gamma _2} \ u_3^{p_2}, \cdots , t^{s_{m}} \ |x|_{\mathbb {G}}^{\gamma _{m}} \ u_1^{p_{m}} \right) , \end{aligned}\) H ( x , t , u ) = t s 1 | x | G γ 1 u 2 p 1 , t s 2 | x | G γ 2 u 3 p 2 , , t s m | x | G γ m u 1 p m , with \(p_i \ge 1\) p i 1 , \(\textstyle \prod _{i=1}^m p_i>1\) i = 1 m p i > 1 , \(\gamma _i\ge 0\) γ i 0 , \(s_i> -1\) s i > - 1 for \(i =1, \cdots , m\) i = 1 , , m , where \(|\cdot |_{\mathbb {G}}\) | · | G denotes a homogeneous norm on \(\mathbb {G}\) G . We determine the Fujita-type exponent for this system, which depends on the homogeneous dimension Q of \(\mathbb {G}\) G . In contrast to previous studies, our results are obtained by iterative methods involving the symmetric submarkovian semigroup associated with the operator \(\Delta _{\mathbb {G}}\) Δ G . In particular, the derivation of the blow-up result is delicate and is carried out through a novel approach based on Stirling’s asymptotic formula.