<p>We consider the Dirichlet problems <Equation ID="Equ34"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_524_Article_Equ34.gif" Format="GIF" Height="75" Rendition="HTML" Resolution="72" Type="Linedraw" Width="364" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} - \textrm{div} \Bigg ( \,\Big ( |\nabla u_{p}| -1 \Big )_{+}^{p-1} \displaystyle { \frac{\nabla u_{p}}{|\nabla u_{p}|} } \Bigg ) = f &amp; \quad \text { in } B_R \qquad \\ u_{p}=0 \, &amp; \quad \text { on } \partial {B_R}, \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <mrow> <mo>-</mo> <mtext>div</mtext> <mrow> <mo maxsize="2.470em" minsize="2.470em" stretchy="true">(</mo> </mrow> <mspace width="0.166667em" /> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">(</mo> </mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> </mrow> <msub> <mi>u</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">|</mo> <mo>-</mo> <mn>1</mn> </mrow> <msubsup> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">)</mo> </mrow> <mrow> <mo>+</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msubsup> <mfrac> <mrow> <mi mathvariant="normal">∇</mi> <msub> <mi>u</mi> <mi>p</mi> </msub> </mrow> <mrow> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> </mrow> <msub> <mi>u</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">|</mo> </mrow> </mrow> </mfrac> <mrow> <mo maxsize="2.470em" minsize="2.470em" stretchy="true">)</mo> </mrow> <mo>=</mo> <mi>f</mi> </mrow> </mstyle> </mtd> <mtd columnalign="left"> <mrow> <mspace width="1em" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msub> <mi>B</mi> <mi>R</mi> </msub> <mspace width="2em" /> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>u</mi> <mi>p</mi> </msub> <mo>=</mo> <mn>0</mn> <mspace width="0.166667em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="1em" /> <mspace width="0.333333em" /> <mtext>on</mtext> <mspace width="0.333333em" /> <mi>∂</mi> <msub> <mi>B</mi> <mi>R</mi> </msub> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_524_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(p &gt; 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_524_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="125" /> </InlineMediaObject> <EquationSource Format="TEX">\(B_R \subseteq \mathbb {R}^N, \, N\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>B</mi> <mi>R</mi> </msub> <mo>⊆</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> <mspace width="0.166667em" /> <mi>N</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, is the open ball centered at the origin with radius <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_524_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\(R&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>R</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Through a well-known result by Talenti (Annali di Matematica 120:159–184, 1979), we explicitly express the gradient of the solution <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_524_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(u_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation> outside the set <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_524_Article_IEq5.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="94" /> </InlineMediaObject> <EquationSource Format="TEX">\(\{ |\nabla u_p|\le 1\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">{</mo> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> <msub> <mi>u</mi> <mi>p</mi> </msub> <mo stretchy="false">|</mo> <mo>≤</mo> <mn>1</mn> <mo stretchy="false">}</mo> </mrow> </math></EquationSource> </InlineEquation>, if the datum <i>f</i> is a non-negative integrable radially decreasing function. This allows us to establish some sharp higher regularity results for the weak solutions, assuming that the datum <i>f</i> belongs to a suitable Lorentz space, i.e. under a weaker assumption on the datum with respect to the available literature. Moreover we analyze the behaviour of <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_524_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(u_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13163_2025_524_Article_IEq7.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(p \rightarrow 1^+\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">→</mo> <msup> <mn>1</mn> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

On widely degenerate p-Laplace equations with symmetric data

  • Stefania Russo

摘要

We consider the Dirichlet problems \(\begin{aligned} {\left\{ \begin{array}{ll} - \textrm{div} \Bigg ( \,\Big ( |\nabla u_{p}| -1 \Big )_{+}^{p-1} \displaystyle { \frac{\nabla u_{p}}{|\nabla u_{p}|} } \Bigg ) = f & \quad \text { in } B_R \qquad \\ u_{p}=0 \, & \quad \text { on } \partial {B_R}, \end{array}\right. } \end{aligned}\) - div ( ( | u p | - 1 ) + p - 1 u p | u p | ) = f in B R u p = 0 on B R , where \(p > 1\) p > 1 and \(B_R \subseteq \mathbb {R}^N, \, N\ge 2\) B R R N , N 2 , is the open ball centered at the origin with radius \(R>0\) R > 0 . Through a well-known result by Talenti (Annali di Matematica 120:159–184, 1979), we explicitly express the gradient of the solution \(u_p\) u p outside the set \(\{ |\nabla u_p|\le 1\}\) { | u p | 1 } , if the datum f is a non-negative integrable radially decreasing function. This allows us to establish some sharp higher regularity results for the weak solutions, assuming that the datum f belongs to a suitable Lorentz space, i.e. under a weaker assumption on the datum with respect to the available literature. Moreover we analyze the behaviour of \(u_p\) u p as \(p \rightarrow 1^+\) p 1 + .