<p>We are concerned with the existence and concentrating behavior of positive ground state solutions for a quasilinear Kirchhoff equation involving critical Sobolev exponent with competing potentials <Equation ID="Equ72"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1215_Article_Equ72.gif" Format="GIF" Height="67" Rendition="HTML" Resolution="72" Type="Linedraw" Width="524" /> </MediaObject> <EquationSource Format="TEX">\( \begin{gathered} \left( \epsilon ^2a+\epsilon b\int _{\mathbb {R}^3}g^2(u)|\nabla u|^2\textrm{d}x\right) \left[ -\text {div}(g^2(u)\nabla u)+ g(u)g^{\prime }(u)|\nabla u|^2\right] +V( x)u\\ \ \ \ \ \ \ =Q( x)h(u)+K( x)|G(u)|^{4}G(u)g(u),~x\in \mathbb {R}^3,\\ \end{gathered} \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd> <mrow> <mfenced close=")" open="("> <msup> <mi>ϵ</mi> <mn>2</mn> </msup> <mi>a</mi> <mo>+</mo> <mi>ϵ</mi> <mi>b</mi> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </msub> <msup> <mi>g</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mtext>d</mtext> <mi>x</mi> </mfenced> <mfenced close="]" open="["> <mo>-</mo> <mi mathvariant="normal">div</mi> <mrow> <mo stretchy="false">(</mo> <msup> <mi mathvariant="normal">g</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">u</mi> <mo stretchy="false">)</mo> </mrow> <mi mathvariant="normal">∇</mi> <mi mathvariant="normal">u</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi mathvariant="normal">g</mi> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">u</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mi mathvariant="normal">g</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">u</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> <mi mathvariant="normal">u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> </mfenced> <mo>+</mo> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> </mrow> </mtd> </mtr> <mtr> <mtd> <mrow> <mrow /> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="4pt" /> <mo>=</mo> <mi>Q</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>h</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <msup> <mrow> <mi>K</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> <mi>G</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> </mrow> <mn>4</mn> </msup> <mi>G</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="3.33333pt" /> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd> <mrow /> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1215_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(a,b&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>,</mo> <mi>b</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> are constants, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1215_Article_IEq2.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϵ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is a small parameter, and <i>g</i> is an even differential function related to the quasilinear term, such that <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1215_Article_IEq3.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="122" /> </InlineMediaObject> <EquationSource Format="TEX">\(G(t)=\int _0^tg(s)\textrm{d}s\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msubsup> <mo>∫</mo> <mn>0</mn> <mi>t</mi> </msubsup> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> <mtext>d</mtext> <mi>s</mi> </mrow> </math></EquationSource> </InlineEquation>. Under some suitable assumptions on <i>V</i>,&#xa0;<i>Q</i>,&#xa0;<i>K</i> and <i>h</i>, we conclude that this equation admits a positive ground state solution for all sufficiently small <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1215_Article_IEq2.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϵ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> using variational methods, where the decay rate of the obtained solution as <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1215_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="80" /> </InlineMediaObject> <EquationSource Format="TEX">\(|x|\rightarrow +\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> <mo stretchy="false">→</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> and its concentration on the set of minimal points of <i>V</i> and the sets of maximal points of <i>Q</i> and <i>K</i> as <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1215_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon \rightarrow 0^+\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϵ</mi> <mo stretchy="false">→</mo> <msup> <mn>0</mn> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> are also considered. In particular, we also investigate the nonexistence of ground state solutions.</p>

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Concentration of ground states for quasilinear Kirchhoff type equations at critical growth

  • Liejun Shen,
  • Marco Squassina

摘要

We are concerned with the existence and concentrating behavior of positive ground state solutions for a quasilinear Kirchhoff equation involving critical Sobolev exponent with competing potentials \( \begin{gathered} \left( \epsilon ^2a+\epsilon b\int _{\mathbb {R}^3}g^2(u)|\nabla u|^2\textrm{d}x\right) \left[ -\text {div}(g^2(u)\nabla u)+ g(u)g^{\prime }(u)|\nabla u|^2\right] +V( x)u\\ \ \ \ \ \ \ =Q( x)h(u)+K( x)|G(u)|^{4}G(u)g(u),~x\in \mathbb {R}^3,\\ \end{gathered} \) ϵ 2 a + ϵ b R 3 g 2 ( u ) | u | 2 d x - div ( g 2 ( u ) u ) + g ( u ) g ( u ) | u | 2 + V ( x ) u = Q ( x ) h ( u ) + K ( x ) | G ( u ) | 4 G ( u ) g ( u ) , x R 3 , where \(a,b>0\) a , b > 0 are constants, \(\epsilon >0\) ϵ > 0 is a small parameter, and g is an even differential function related to the quasilinear term, such that \(G(t)=\int _0^tg(s)\textrm{d}s\) G ( t ) = 0 t g ( s ) d s . Under some suitable assumptions on VQK and h, we conclude that this equation admits a positive ground state solution for all sufficiently small \(\epsilon >0\) ϵ > 0 using variational methods, where the decay rate of the obtained solution as \(|x|\rightarrow +\infty \) | x | + and its concentration on the set of minimal points of V and the sets of maximal points of Q and K as \(\epsilon \rightarrow 0^+\) ϵ 0 + are also considered. In particular, we also investigate the nonexistence of ground state solutions.