<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {G}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">G</mi> </math></EquationSource> </InlineEquation> be a graded Lie group with homogeneous dimension <i>Q</i>. In this paper, we study the Cauchy problem for a semilinear hypoelliptic damped wave equation involving a positive Rockland operator <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathcal {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">R</mi> </math></EquationSource> </InlineEquation> of homogeneous degree <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\nu \geqslant 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ν</mi> <mo>⩾</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> on <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathbb {G}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">G</mi> </math></EquationSource> </InlineEquation> with power type nonlinearity <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(|u|^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation> and initial data taken from negative order homogeneous Sobolev space <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\dot{H}^{-\gamma }(\mathbb {G}), \gamma &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mover accent="true"> <mi>H</mi> <mo>˙</mo> </mover> <mrow> <mo>-</mo> <mi>γ</mi> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">G</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mi>γ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. In the framework of Sobolev spaces of negative order, we prove that <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(p_{\text {Crit}}(Q, \gamma , \nu ):=1+\frac{2\nu }{Q+2\gamma }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>p</mi> <mtext>Crit</mtext> </msub> <mrow> <mo stretchy="false">(</mo> <mi>Q</mi> <mo>,</mo> <mi>γ</mi> <mo>,</mo> <mi>ν</mi> <mo stretchy="false">)</mo> </mrow> <mo>:</mo> <mo>=</mo> <mn>1</mn> <mo>+</mo> <mfrac> <mrow> <mn>2</mn> <mi>ν</mi> </mrow> <mrow> <mi>Q</mi> <mo>+</mo> <mn>2</mn> <mi>γ</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation> is the new critical exponent for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\gamma \in (0, \frac{Q}{2})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>γ</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mfrac> <mi>Q</mi> <mn>2</mn> </mfrac> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. More precisely, we show the global-in-time existence of small data Sobolev solutions of lower regularity for <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(p&gt;p_{\text {Crit}}(Q, \gamma , \nu ) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&gt;</mo> <msub> <mi>p</mi> <mtext>Crit</mtext> </msub> <mrow> <mo stretchy="false">(</mo> <mi>Q</mi> <mo>,</mo> <mi>γ</mi> <mo>,</mo> <mi>ν</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> in the energy evolution space <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\( \mathcal {C}\left( [0, T], H^{s}(\mathbb {G})\right) , s\in (0, 1]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">C</mi> <mfenced close=")" open="("> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">]</mo> </mrow> <mo>,</mo> <msup> <mi>H</mi> <mi>s</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">G</mi> <mo stretchy="false">)</mo> </mrow> </mfenced> <mo>,</mo> <mi>s</mi> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. Under certain conditions on the initial data, we also prove a finite-time blow-up of weak solutions for <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(1&lt;p&lt;p_{\text {Crit}}(Q, \gamma , \nu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <msub> <mi>p</mi> <mtext>Crit</mtext> </msub> <mrow> <mo stretchy="false">(</mo> <mi>Q</mi> <mo>,</mo> <mi>γ</mi> <mo>,</mo> <mi>ν</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. Furthermore, to precisely characterize the blow-up time, we derive sharp upper bound and lower bound estimates for the lifespan in the subcritical cases. We emphasize that our results are also new, even in the setting of higher-order differential operators on <InlineEquation ID="IEq12"> <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>, and more generally, on stratified Lie groups.</p>

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Higher order hypoelliptic damped wave equations on graded Lie groups with data from negative order Sobolev spaces

  • Aparajita Dasgupta,
  • Vishvesh Kumar,
  • Shyam Swarup Mondal,
  • Michael Ruzhansky

摘要

Let \(\mathbb {G}\) G be a graded Lie group with homogeneous dimension Q. In this paper, we study the Cauchy problem for a semilinear hypoelliptic damped wave equation involving a positive Rockland operator \(\mathcal {R}\) R of homogeneous degree \(\nu \geqslant 2\) ν 2 on \(\mathbb {G}\) G with power type nonlinearity \(|u|^p\) | u | p and initial data taken from negative order homogeneous Sobolev space \(\dot{H}^{-\gamma }(\mathbb {G}), \gamma >0\) H ˙ - γ ( G ) , γ > 0 . In the framework of Sobolev spaces of negative order, we prove that \(p_{\text {Crit}}(Q, \gamma , \nu ):=1+\frac{2\nu }{Q+2\gamma }\) p Crit ( Q , γ , ν ) : = 1 + 2 ν Q + 2 γ is the new critical exponent for \(\gamma \in (0, \frac{Q}{2})\) γ ( 0 , Q 2 ) . More precisely, we show the global-in-time existence of small data Sobolev solutions of lower regularity for \(p>p_{\text {Crit}}(Q, \gamma , \nu ) \) p > p Crit ( Q , γ , ν ) in the energy evolution space \( \mathcal {C}\left( [0, T], H^{s}(\mathbb {G})\right) , s\in (0, 1]\) C [ 0 , T ] , H s ( G ) , s ( 0 , 1 ] . Under certain conditions on the initial data, we also prove a finite-time blow-up of weak solutions for \(1<p<p_{\text {Crit}}(Q, \gamma , \nu )\) 1 < p < p Crit ( Q , γ , ν ) . Furthermore, to precisely characterize the blow-up time, we derive sharp upper bound and lower bound estimates for the lifespan in the subcritical cases. We emphasize that our results are also new, even in the setting of higher-order differential operators on \(\mathbb {R}^n\) R n , and more generally, on stratified Lie groups.