<p>In this paper we extend the classical sub-supersolution Sattinger iteration method to 1-Laplace type boundary value problems of the form <Equation ID="Equ94"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} \displaystyle -\Delta _1 u = F(x,u) &amp; \text {in}\;\Omega ,\\ u=0 &amp; \text {on}\;\partial \Omega , \end{array}\right. } \end{aligned}\)</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> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mn>1</mn> </msub> <mi>u</mi> <mo>=</mo> <mi>F</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mstyle> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="0.277778em" /> <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="0.277778em" /> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation> is an open bounded domain of <InlineEquation ID="IEq2"> <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> (<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(N\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>) with Lipschitz boundary and <i>F</i>(<i>x</i>,&#xa0;<i>s</i>) is a Caratheódory function. This goal is achieved through a perturbation method that overcomes structural obstructions arising from the presence of the 1-Laplacian and by proving a weak comparison principle for these problems. As a significant application of our main result we establish existence and non-existence theorems for the so-called “concave-convex” problem involving the 1-Laplacian as leading term.</p>

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The Sattinger iteration method for 1-Laplace type problems and its application to concave-convex nonlinearities

  • Antonio J. Martínez Aparicio,
  • Francescantonio Oliva,
  • Francesco Petitta

摘要

In this paper we extend the classical sub-supersolution Sattinger iteration method to 1-Laplace type boundary value problems of the form \(\begin{aligned} {\left\{ \begin{array}{ll} \displaystyle -\Delta _1 u = F(x,u) & \text {in}\;\Omega ,\\ u=0 & \text {on}\;\partial \Omega , \end{array}\right. } \end{aligned}\) - Δ 1 u = F ( x , u ) in Ω , u = 0 on Ω , where \(\Omega \) Ω is an open bounded domain of \({\mathbb {R}}^N\) R N ( \(N\ge 2\) N 2 ) with Lipschitz boundary and F(xs) is a Caratheódory function. This goal is achieved through a perturbation method that overcomes structural obstructions arising from the presence of the 1-Laplacian and by proving a weak comparison principle for these problems. As a significant application of our main result we establish existence and non-existence theorems for the so-called “concave-convex” problem involving the 1-Laplacian as leading term.