<p>In this paper, we study the local gradient regularity of non-negative weak solutions to doubly nonlinear parabolic partial differential equations of the type <Equation ID="Equ119"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1076_Article_Equ119.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="277" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \partial _t u^q - {{\,\textrm{div}\,}}A(x,t,Du)=0 \qquad \text{ in }~\Omega _T, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <msup> <mi>u</mi> <mi>q</mi> </msup> <mo>-</mo> <mrow> <mspace width="0.166667em" /> <mtext>div</mtext> <mspace width="0.166667em" /> </mrow> <mi>A</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo>,</mo> <mi>D</mi> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>0</mn> <mspace width="2em" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="3.33333pt" /> <msub> <mi mathvariant="normal">Ω</mi> <mi>T</mi> </msub> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>with&#xa0;<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1076_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(q&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>,&#xa0;<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1076_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="176" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega _T:=\Omega \times (0,T)\subset \mathbb {R}^{n+1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Ω</mi> <mi>T</mi> </msub> <mo>:</mo> <mo>=</mo> <mi mathvariant="normal">Ω</mi> <mo>×</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">)</mo> </mrow> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> a space-time cylinder, and&#xa0;<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1076_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="100" /> </InlineMediaObject> <EquationSource Format="TEX">\(A=A(x,t,\xi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>A</mi> <mo>=</mo> <mi>A</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo>,</mo> <mi>ξ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> a vector field satisfying standard&#xa0;<i>p</i>-growth conditions. Our main result establishes the local Hölder continuity of the spatial gradient of non-negative weak solutions in the super-critical fast diffusion regime <Equation ID="Equ120"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1076_Article_Equ120.gif" Format="GIF" Height="43" Rendition="HTML" Resolution="72" Type="Linedraw" Width="192" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} 0&lt;p-1&lt;q&lt;\frac{n(p-1)}{(n-p)_+}. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <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> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>This result is achieved by utilizing a time-insensitive Harnack inequality and Schauder estimates that are developed for equations of parabolic&#xa0;<i>p</i>-Laplacian type. Additionally, we establish a local <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1076_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>∞</mi> </msup> </math></EquationSource> </InlineEquation>-bound for the spatial gradient.</p>

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Gradient regularity for a class of doubly nonlinear parabolic partial differential equations

  • Michael Strunk

摘要

In this paper, we study the local gradient regularity of non-negative weak solutions to doubly nonlinear parabolic partial differential equations of the type \(\begin{aligned} \partial _t u^q - {{\,\textrm{div}\,}}A(x,t,Du)=0 \qquad \text{ in }~\Omega _T, \end{aligned}\) t u q - div A ( x , t , D u ) = 0 in Ω T , with  \(q>0\) q > 0 \(\Omega _T:=\Omega \times (0,T)\subset \mathbb {R}^{n+1}\) Ω T : = Ω × ( 0 , T ) R n + 1 a space-time cylinder, and  \(A=A(x,t,\xi )\) A = A ( x , t , ξ ) a vector field satisfying standard p-growth conditions. Our main result establishes the local Hölder continuity of the spatial gradient of non-negative weak solutions in the super-critical fast diffusion regime \(\begin{aligned} 0<p-1<q<\frac{n(p-1)}{(n-p)_+}. \end{aligned}\) 0 < p - 1 < q < n ( p - 1 ) ( n - p ) + . This result is achieved by utilizing a time-insensitive Harnack inequality and Schauder estimates that are developed for equations of parabolic p-Laplacian type. Additionally, we establish a local \(L^\infty \) L -bound for the spatial gradient.