<p>We are concerned with the existence of global and blow-up solutions for the nonlinear parabolic problem described by the Hardy-Hénon equation <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(u_t - \Delta _{\mathbb {H}} u = |\cdot |_{\mathbb {H}}^{\gamma } u^p \text{ in } \mathbb {H}^N \times (0,T),\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi mathvariant="double-struck">H</mi> </msub> <mi>u</mi> <mo>=</mo> <msubsup> <mrow> <mo stretchy="false">|</mo> <mo>·</mo> <mo stretchy="false">|</mo> </mrow> <mrow> <mi mathvariant="double-struck">H</mi> </mrow> <mi>γ</mi> </msubsup> <msup> <mi>u</mi> <mi>p</mi> </msup> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msup> <mrow> <mi mathvariant="double-struck">H</mi> </mrow> <mi>N</mi> </msup> <mo>×</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {H}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">H</mi> </mrow> <mi>N</mi> </msup> </math></EquationSource> </InlineEquation> is the <i>N</i>-dimensional Heisenberg group, and the singular term <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(|\cdot |_{\mathbb {H}}^{\gamma }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mo stretchy="false">|</mo> <mo>·</mo> <mo stretchy="false">|</mo> </mrow> <mrow> <mi mathvariant="double-struck">H</mi> </mrow> <mi>γ</mi> </msubsup> </math></EquationSource> </InlineEquation> is given by the Korányi norm. Our study focuses on nonnegative solutions. We establish that for <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\gamma \ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>γ</mi> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, the Fujita critical exponent is <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(p_c = 1+ (2+\gamma )/Q\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>p</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>1</mn> <mo>+</mo> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mo>+</mo> <mi>γ</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">/</mo> <mi>Q</mi> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(Q=2N+2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>Q</mi> <mo>=</mo> <mn>2</mn> <mi>N</mi> <mo>+</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> is the homogeneous dimension of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathbb {H}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">H</mi> </mrow> <mi>N</mi> </msup> </math></EquationSource> </InlineEquation>. For <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(-2&lt;\gamma &lt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mn>2</mn> <mo>&lt;</mo> <mi>γ</mi> <mo>&lt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, the solutions blow up for <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(1&lt;p\le 1+ (2+\gamma )/Q\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>≤</mo> <mn>1</mn> <mo>+</mo> <mo stretchy="false">(</mo> <mn>2</mn> <mo>+</mo> <mi>γ</mi> <mo stretchy="false">)</mo> <mo stretchy="false">/</mo> <mi>Q</mi> </mrow> </math></EquationSource> </InlineEquation>, while global solutions exist for <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(p&gt;1+ (2+\gamma )/(Q + \gamma )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&gt;</mo> <mn>1</mn> <mo>+</mo> <mo stretchy="false">(</mo> <mn>2</mn> <mo>+</mo> <mi>γ</mi> <mo stretchy="false">)</mo> <mo stretchy="false">/</mo> <mo stretchy="false">(</mo> <mi>Q</mi> <mo>+</mo> <mi>γ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. In particular, our results coincide with the results found by Georgiev and Palmieri in [<CitationRef CitationID="CR17">17</CitationRef>].</p>

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Blow-up and global mild solutions for a Hardy-Hénon parabolic equation on the Heisenberg group

  • Ricardo Castillo,
  • Ricardo Freire,
  • Miguel Loayza

摘要

We are concerned with the existence of global and blow-up solutions for the nonlinear parabolic problem described by the Hardy-Hénon equation \(u_t - \Delta _{\mathbb {H}} u = |\cdot |_{\mathbb {H}}^{\gamma } u^p \text{ in } \mathbb {H}^N \times (0,T),\) u t - Δ H u = | · | H γ u p in H N × ( 0 , T ) , where \(\mathbb {H}^N\) H N is the N-dimensional Heisenberg group, and the singular term \(|\cdot |_{\mathbb {H}}^{\gamma }\) | · | H γ is given by the Korányi norm. Our study focuses on nonnegative solutions. We establish that for \(\gamma \ge 0\) γ 0 , the Fujita critical exponent is \(p_c = 1+ (2+\gamma )/Q\) p c = 1 + ( 2 + γ ) / Q , where \(Q=2N+2\) Q = 2 N + 2 is the homogeneous dimension of \(\mathbb {H}^N\) H N . For \(-2<\gamma <0\) - 2 < γ < 0 , the solutions blow up for \(1<p\le 1+ (2+\gamma )/Q\) 1 < p 1 + ( 2 + γ ) / Q , while global solutions exist for \(p>1+ (2+\gamma )/(Q + \gamma )\) p > 1 + ( 2 + γ ) / ( Q + γ ) . In particular, our results coincide with the results found by Georgiev and Palmieri in [17].