<p>In this paper we analyze the asymptotic behaviour as <InlineEquation ID="IEq3"> <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> of solutions <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(u_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation> to <Equation ID="Equ5"> <EquationSource Format="TEX">\( \left\{ \begin{array}{rclr} -\Delta _pu_p&amp; =&amp; \lambda |\nabla u_p|^{p-2}\nabla u_p\cdot \frac{x}{|x|^2}+ f&amp; \quad \text{ in } \Omega ,\\ u_p&amp; =&amp; 0 &amp; \quad \text{ on } \partial \Omega , \end{array}\right. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>p</mi> </msub> <msub> <mi>u</mi> <mi>p</mi> </msub> </mrow> </mtd> <mtd> <mo>=</mo> </mtd> <mtd columnalign="left"> <mrow> <mrow> <mi>λ</mi> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> </mrow> <msub> <mi>u</mi> <mi>p</mi> </msub> <msup> <mrow> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi mathvariant="normal">∇</mi> <msub> <mi>u</mi> <mi>p</mi> </msub> <mo>·</mo> <mfrac> <mi>x</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> </mfrac> <mo>+</mo> <mi>f</mi> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mspace width="1em" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <msub> <mi>u</mi> <mi>p</mi> </msub> </mrow> </mtd> <mtd> <mo>=</mo> </mtd> <mtd columnalign="left"> <mn>0</mn> </mtd> <mtd columnalign="right"> <mrow> <mspace width="1em" /> <mspace width="0.333333em" /> <mtext>on</mtext> <mspace width="0.333333em" /> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>where <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation> is a bounded open subset of <InlineEquation ID="IEq6"> <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> with Lipschitz boundary containing the origin, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\lambda \in \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, and <i>f</i> is a nonnegative datum in <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(L^{N,\infty }(\Omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mrow> <mi>N</mi> <mo>,</mo> <mi>∞</mi> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. As a consequence, under suitable smallness assumptions on <i>f</i> and <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>, we show sharp existence results of bounded solutions to the Dirichlet problems <Equation ID="Equ6"> <EquationSource Format="TEX">\({\left\{ \begin{array}{ll} \displaystyle - \Delta _{1} u = \lambda \frac{D u}{|D u|}\cdot \frac{x}{|x|^2}+f &amp; \text {in}\, \Omega , \\ u=0 &amp; \text {on}\ \partial \Omega , \end{array}\right. } \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mn>1</mn> </msub> <mi>u</mi> <mo>=</mo> <mi>λ</mi> <mfrac> <mrow> <mi mathvariant="italic">Du</mi> </mrow> <mrow> <mo stretchy="false">|</mo> <mi>D</mi> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> </mfrac> <mo>·</mo> <mfrac> <mi>x</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> </mfrac> <mo>+</mo> <mi>f</mi> </mrow> </mstyle> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="0.166667em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mo>=</mo> <mn>0</mn> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>on</mtext> <mspace width="4pt" /> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>where <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\displaystyle \Delta _{1}u=\hbox {div}\,\left( \frac{Du}{|Du|}\right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mn>1</mn> </msub> <mi>u</mi> <mo>=</mo> <mtext>div</mtext> <mspace width="0.166667em" /> <mfenced close=")" open="("> <mfrac> <mrow> <mi mathvariant="italic">Du</mi> </mrow> <mrow> <mo stretchy="false">|</mo> <mi>D</mi> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> </mfrac> </mfenced> </mrow> </mstyle> </math></EquationSource> </InlineEquation> is the 1-Laplacian operator. The case of a generic drift term in <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(L^{N,\infty }(\Omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mrow> <mi>N</mi> <mo>,</mo> <mi>∞</mi> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is also considered. Explicits examples are given in order to show the optimality of the main assumptions on the data.</p>

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Existence, Non-Existence and Degeneracy of Limit Solutions to p-Laplace Problems Involving Hardy Potentials as \(p\rightarrow 1^+\). The Case of A Critical Drift

  • Juan Carlos Ortiz Chata,
  • Francesco Petitta

摘要

In this paper we analyze the asymptotic behaviour as \(p\rightarrow 1^+\) p 1 + of solutions \(u_p\) u p to \( \left\{ \begin{array}{rclr} -\Delta _pu_p& =& \lambda |\nabla u_p|^{p-2}\nabla u_p\cdot \frac{x}{|x|^2}+ f& \quad \text{ in } \Omega ,\\ u_p& =& 0 & \quad \text{ on } \partial \Omega , \end{array}\right. \) - Δ p u p = λ | u p | p - 2 u p · x | x | 2 + f in Ω , u p = 0 on Ω , where \(\Omega \) Ω is a bounded open subset of \(\mathbb {R}^N\) R N with Lipschitz boundary containing the origin, \(\lambda \in \mathbb {R}\) λ R , and f is a nonnegative datum in \(L^{N,\infty }(\Omega )\) L N , ( Ω ) . As a consequence, under suitable smallness assumptions on f and \(\lambda \) λ , we show sharp existence results of bounded solutions to the Dirichlet problems \({\left\{ \begin{array}{ll} \displaystyle - \Delta _{1} u = \lambda \frac{D u}{|D u|}\cdot \frac{x}{|x|^2}+f & \text {in}\, \Omega , \\ u=0 & \text {on}\ \partial \Omega , \end{array}\right. } \) - Δ 1 u = λ Du | D u | · x | x | 2 + f in Ω , u = 0 on Ω , where \(\displaystyle \Delta _{1}u=\hbox {div}\,\left( \frac{Du}{|Du|}\right) \) Δ 1 u = div Du | D u | is the 1-Laplacian operator. The case of a generic drift term in \(L^{N,\infty }(\Omega )\) L N , ( Ω ) is also considered. Explicits examples are given in order to show the optimality of the main assumptions on the data.