<p>In this paper, we are concerned with the existence and multiplicity of multi-bump solutions for the following (<i>N</i>,&#xa0;<i>q</i>)-Laplacian equation <Equation ID="Equ45"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2062_Article_Equ45.gif" Format="GIF" Height="46" Rendition="HTML" Resolution="72" Type="Linedraw" Width="373" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} &amp; -\Delta _N u-\Delta _q u+(\mu \mathcal {V}(x)+\mathcal {Z}(x))(|u|^{N-2}u+|u|^{q-2}u)\\ &amp; \quad =h(u)+|u|^{q-2}u\log |u|^q\quad \text {in}\ \mathbb {R}^N, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd /> <mtd columnalign="left"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>N</mi> </msub> <mi>u</mi> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>q</mi> </msub> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>μ</mi> <mi mathvariant="script">V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi mathvariant="script">Z</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mrow> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow /> </mtd> <mtd columnalign="left"> <mrow> <mspace width="1em" /> <mo>=</mo> <mi>h</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>log</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mi>q</mi> </msup> <mspace width="1em" /> <mtext>in</mtext> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2062_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="80" /> </InlineMediaObject> <EquationSource Format="TEX">\(2\le N&lt;q\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>≤</mo> <mi>N</mi> <mo>&lt;</mo> <mi>q</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2062_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="89" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu \in [1,+\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>1</mn> <mo>,</mo> <mo>+</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2062_Article_IEq5.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="165" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _\mathfrak {s}u=\text {div}(|\nabla u|^{\mathfrak {s}-2}\nabla u)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mi mathvariant="fraktur">s</mi> </msub> <mi>u</mi> <mo>=</mo> <msup> <mrow> <mtext>div</mtext> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi mathvariant="fraktur">s</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mrow> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is the <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2062_Article_IEq6.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="9" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathfrak {s}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="fraktur">s</mi> </math></EquationSource> </InlineEquation>-Laplace operator with <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2062_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="81" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathfrak {s}\in \{N,q\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">s</mi> <mo>∈</mo> <mo stretchy="false">{</mo> <mi>N</mi> <mo>,</mo> <mi>q</mi> <mo stretchy="false">}</mo> </mrow> </math></EquationSource> </InlineEquation>, <i>h</i> is a continuous function with exponential critical growth, <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2062_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {V}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">V</mi> </math></EquationSource> </InlineEquation> is a nonnegative continuous function with the potential well <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2062_Article_IEq9.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="119" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega :=\text {int}(\mathcal {V}^{-1}(0))\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>:</mo> <mo>=</mo> <mtext>int</mtext> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="script">V</mi> </mrow> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> consisting of <i>k</i> components, and the nonnegative continuous function <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2062_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {Z}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">Z</mi> </math></EquationSource> </InlineEquation> verifies some assumptions. With the aid of variational methods, we obtain the existence and multiplicity of multi-bump solutions as <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2062_Article_IEq11.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>μ</mi> </math></EquationSource> </InlineEquation> is large enough. As far as we know, it is the first time that the existence and multiplicity of multi-bump solutions to the (<i>N</i>,&#xa0;<i>q</i>)-Laplacian equation with exponential critical growth and logarithmic nonlinearity are studied. The most obvious and important feature is that we establish some new technique results to prove our results.</p>

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On the Multi-Bump Solutions to (Nq)-Laplacian Equations with Exponential Critical Growth and Logarithmic Nonlinearity in \(\mathbb {R}^N\)

  • Yuxuan Tong,
  • Sihua Liang

摘要

In this paper, we are concerned with the existence and multiplicity of multi-bump solutions for the following (Nq)-Laplacian equation \(\begin{aligned} & -\Delta _N u-\Delta _q u+(\mu \mathcal {V}(x)+\mathcal {Z}(x))(|u|^{N-2}u+|u|^{q-2}u)\\ & \quad =h(u)+|u|^{q-2}u\log |u|^q\quad \text {in}\ \mathbb {R}^N, \end{aligned}\) - Δ N u - Δ q u + ( μ V ( x ) + Z ( x ) ) ( | u | N - 2 u + | u | q - 2 u ) = h ( u ) + | u | q - 2 u log | u | q in R N , where \(2\le N<q\) 2 N < q , \(\mu \in [1,+\infty )\) μ [ 1 , + ) , \(\Delta _\mathfrak {s}u=\text {div}(|\nabla u|^{\mathfrak {s}-2}\nabla u)\) Δ s u = div ( | u | s - 2 u ) is the \(\mathfrak {s}\) s -Laplace operator with \(\mathfrak {s}\in \{N,q\}\) s { N , q } , h is a continuous function with exponential critical growth, \(\mathcal {V}\) V is a nonnegative continuous function with the potential well \(\Omega :=\text {int}(\mathcal {V}^{-1}(0))\) Ω : = int ( V - 1 ( 0 ) ) consisting of k components, and the nonnegative continuous function \(\mathcal {Z}\) Z verifies some assumptions. With the aid of variational methods, we obtain the existence and multiplicity of multi-bump solutions as \(\mu \) μ is large enough. As far as we know, it is the first time that the existence and multiplicity of multi-bump solutions to the (Nq)-Laplacian equation with exponential critical growth and logarithmic nonlinearity are studied. The most obvious and important feature is that we establish some new technique results to prove our results.