<p>We consider non-negative, weak solutions to the doubly nonlinear parabolic equation <Equation ID="Equ51"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="30_2024_1022_Article_Equ51.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="217" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \partial _t \left( u^q\right) -\operatorname {div}\left( |Du|^{p-2}Du\right) =0 \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mfenced close=")" open="("> <msup> <mi>u</mi> <mi>q</mi> </msup> </mfenced> <mo>-</mo> <mo>div</mo> <mfenced close=")" open="("> <msup> <mrow> <mo stretchy="false">|</mo> <mi>D</mi> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>D</mi> <mi>u</mi> </mfenced> <mo>=</mo> <mn>0</mn> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>in the super-critical fast diffusion regime <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2024_1022_Article_IEq1.gif" Format="GIF" Height="43" Rendition="HTML" Resolution="72" Type="Linedraw" Width="191" /> </InlineMediaObject> <EquationSource Format="TEX">\(\displaystyle 0&lt;p-1&lt;q&lt;\frac{N(p-1)}{(N-p)_+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>p</mi> <mo>-</mo> <mn>1</mn> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mfrac> <mrow> <mi>N</mi> <mo stretchy="false">(</mo> <mi>p</mi> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <msub> <mrow> <mo stretchy="false">(</mo> <mi>N</mi> <mo>-</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> </msub> </mfrac> </mrow> </mstyle> </math></EquationSource> </InlineEquation>. We show that when solutions vanish continuously at the Lipschitz boundary of a parabolic cylinder <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2024_1022_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega _T\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Ω</mi> <mi>T</mi> </msub> </math></EquationSource> </InlineEquation>, they satisfy proper Carleson estimates. Assuming further regularity for the boundary of the domain <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2024_1022_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega _T\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Ω</mi> <mi>T</mi> </msub> </math></EquationSource> </InlineEquation>, we obtain a power-like decay at the boundary and a boundary Harnack inequality.</p>

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Boundary estimates for doubly nonlinear parabolic equations

  • Ugo Gianazza,
  • David Jesus

摘要

We consider non-negative, weak solutions to the doubly nonlinear parabolic equation \(\begin{aligned} \partial _t \left( u^q\right) -\operatorname {div}\left( |Du|^{p-2}Du\right) =0 \end{aligned}\) t u q - div | D u | p - 2 D u = 0 in the super-critical fast diffusion regime \(\displaystyle 0<p-1<q<\frac{N(p-1)}{(N-p)_+}\) 0 < p - 1 < q < N ( p - 1 ) ( N - p ) + . We show that when solutions vanish continuously at the Lipschitz boundary of a parabolic cylinder \(\Omega _T\) Ω T , they satisfy proper Carleson estimates. Assuming further regularity for the boundary of the domain \(\Omega _T\) Ω T , we obtain a power-like decay at the boundary and a boundary Harnack inequality.