<p>The purpose of this paper is to study the following singularly perturbed <i>N</i>-Laplacian Kirchhoff-type equation: <Equation ID="Equ87"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="229_2024_1611_Article_Equ87.gif" Format="GIF" Height="74" Rendition="HTML" Resolution="72" Type="Linedraw" Width="529" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{aligned}&amp;-\left( \varepsilon ^{N}+\varepsilon ^{N} b\int _{ \mathbb {R}^{N}}|\nabla v|^{N} \textrm{d}x \right) \Delta _{N} v+V(x)|v|^{N-2}v=Q(x)f(v),&amp;x\in \mathbb {R}^{N},\\&amp;v\in W^{1,N}(\mathbb {R}^{N}), \end{aligned} \right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd /> <mtd columnalign="left"> <mrow> <mo>-</mo> <mfenced close=")" open="("> <msup> <mi>ε</mi> <mi>N</mi> </msup> <mo>+</mo> <msup> <mi>ε</mi> <mi>N</mi> </msup> <mi>b</mi> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mi>N</mi> </msup> <mtext>d</mtext> <mi>x</mi> </mfenced> <msub> <mi mathvariant="normal">Δ</mi> <mi>N</mi> </msub> <mi>v</mi> <mo>+</mo> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>v</mi> <mo>=</mo> <mi>Q</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow /> </mtd> <mtd columnalign="left"> <mrow> <mi>v</mi> <mo>∈</mo> <msup> <mi>W</mi> <mrow> <mn>1</mn> <mo>,</mo> <mi>N</mi> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="229_2024_1611_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(N\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, <i>b</i> is a positive constant, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="229_2024_1611_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _{N}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mi>N</mi> </msub> </math></EquationSource> </InlineEquation> is the <i>N</i>-Laplacian operator, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="229_2024_1611_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ε</mi> </math></EquationSource> </InlineEquation> is a positive parameter, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="229_2024_1611_Article_IEq4.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="123" /> </InlineMediaObject> <EquationSource Format="TEX">\(V,Q\in {\mathcal {C}}\left( \mathbb {R}^N, \mathbb {R}\right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo>,</mo> <mi>Q</mi> <mo>∈</mo> <mi mathvariant="script">C</mi> <mfenced close=")" open="("> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> <mi mathvariant="double-struck">R</mi> </mfenced> </mrow> </math></EquationSource> </InlineEquation> and <i>f</i> has critical exponential growth at infinity. In order to overcome difficulties due to lack of compactness aroused by the critical exponential growth of <i>f</i> and quasilinear characteristic of the equation, we develop some delicate analyses to give a fine threshold of the Mountain-Pass minimax level and show the existence and concentration of semiclassical ground state solutions for the above equation. In particular, if <i>V</i> remains constant, the concentration occurs at the maximum point set of <i>Q</i>.</p>

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Concentration of semiclassical ground states for a N-Laplacian Kirchhoff-type problem with critical exponential growth

  • Die Hu,
  • Dongdong Qin,
  • Xianhua Tang

摘要

The purpose of this paper is to study the following singularly perturbed N-Laplacian Kirchhoff-type equation: \(\begin{aligned} \left\{ \begin{aligned}&-\left( \varepsilon ^{N}+\varepsilon ^{N} b\int _{ \mathbb {R}^{N}}|\nabla v|^{N} \textrm{d}x \right) \Delta _{N} v+V(x)|v|^{N-2}v=Q(x)f(v),&x\in \mathbb {R}^{N},\\&v\in W^{1,N}(\mathbb {R}^{N}), \end{aligned} \right. \end{aligned}\) - ε N + ε N b R N | v | N d x Δ N v + V ( x ) | v | N - 2 v = Q ( x ) f ( v ) , x R N , v W 1 , N ( R N ) , where \(N\ge 2\) N 2 , b is a positive constant, \(\Delta _{N}\) Δ N is the N-Laplacian operator, \(\varepsilon \) ε is a positive parameter, \(V,Q\in {\mathcal {C}}\left( \mathbb {R}^N, \mathbb {R}\right) \) V , Q C R N , R and f has critical exponential growth at infinity. In order to overcome difficulties due to lack of compactness aroused by the critical exponential growth of f and quasilinear characteristic of the equation, we develop some delicate analyses to give a fine threshold of the Mountain-Pass minimax level and show the existence and concentration of semiclassical ground state solutions for the above equation. In particular, if V remains constant, the concentration occurs at the maximum point set of Q.