<p>In this paper, we consider the following double phase problem with combined power nonlinearities and multiple potentials <Equation ID="Equ81"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_Equ81.gif" Format="GIF" Height="48" Rendition="HTML" Resolution="72" Type="Linedraw" Width="347" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} &amp; -\Delta _p u-\Delta _q u+V(x)(|u|^{p-2}u+|u|^{q-2}u)\\ &amp; \quad =\lambda |u|^{p-2}u+\mu (x)|u|^{m-2}u+|u|^{l-2}u,\quad \text {in}\quad {\mathbb {R}}^N \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd /> <mtd columnalign="left"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>p</mi> </msub> <mi>u</mi> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>q</mi> </msub> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</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> <msup> <mrow> <mi>λ</mi> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mi>μ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>m</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>l</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>,</mo> <mspace width="1em" /> <mtext>in</mtext> <mspace width="1em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>having prescribed mass <Equation ID="Equ82"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_Equ82.gif" Format="GIF" Height="41" Rendition="HTML" Resolution="72" Type="Linedraw" Width="119" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \int _{{\mathbb {R}}^N}|u|^p\,dx=c^p, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mi>p</mi> </msup> <mspace width="0.166667em" /> <mi>d</mi> <mi>x</mi> <mo>=</mo> <msup> <mi>c</mi> <mi>p</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="114" /> </InlineMediaObject> <EquationSource Format="TEX">\(1&lt;p&lt;q&lt;N,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mi>N</mi> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq2.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="105" /> </InlineMediaObject> <EquationSource Format="TEX">\(p&lt;m&lt;\frac{Np}{N-p},\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&lt;</mo> <mi>m</mi> <mo>&lt;</mo> <mfrac> <mrow> <mi mathvariant="italic">Np</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mi>p</mi> </mrow> </mfrac> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq3.gif" Format="GIF" Height="27" Rendition="HTML" Resolution="72" Type="Linedraw" Width="128" /> </InlineMediaObject> <EquationSource Format="TEX">\(\frac{q(N+p)}{N}&lt;l&lt;\frac{Np}{N-p},\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mfrac> <mrow> <mi>q</mi> <mo stretchy="false">(</mo> <mi>N</mi> <mo>+</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> <mi>N</mi> </mfrac> <mo>&lt;</mo> <mi>l</mi> <mo>&lt;</mo> <mfrac> <mrow> <mi mathvariant="italic">Np</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mi>p</mi> </mrow> </mfrac> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <i>V</i>(<i>x</i>) is an external potential vanishing at infinity, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu (x)\ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is a competing potential, and the parameter <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq5.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <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> appears as a Lagrange multiplier. Under some mild assumptions on <i>V</i>(<i>x</i>) and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu (x),\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> for the <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-subcritical case <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq8.gif" Format="GIF" Height="33" Rendition="HTML" Resolution="72" Type="Linedraw" Width="125" /> </InlineMediaObject> <EquationSource Format="TEX">\(m\in \left( p,\frac{p(N+p)}{N}\right) ,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>∈</mo> <mfenced close=")" open="("> <mi>p</mi> <mo>,</mo> <mfrac> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mi>N</mi> <mo>+</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> <mi>N</mi> </mfrac> </mfenced> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> we show that there exists <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(c_0&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>c</mi> <mn>0</mn> </msub> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> such that the normalized solution with negative energy can be obtained when <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq10.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\(c\in (0,c_0)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <msub> <mi>c</mi> <mn>0</mn> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. This is achieved by analyzing the relationship between the energy of double phase problem and its limit problem. For the <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-critical case <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq12.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="86" /> </InlineMediaObject> <EquationSource Format="TEX">\(m=\frac{q(N+p)}{N},\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>=</mo> <mfrac> <mrow> <mi>q</mi> <mo stretchy="false">(</mo> <mi>N</mi> <mo>+</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> <mi>N</mi> </mfrac> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> by limiting the range of parameters, we find the existence of positive ground state normalized solutions with the aid of the Pohozaev constraint and using the properties of the energy in relationship with its limit problem. For the <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-supercritical case <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2168_Article_IEq14.gif" Format="GIF" Height="33" Rendition="HTML" Resolution="72" Type="Linedraw" Width="145" /> </InlineMediaObject> <EquationSource Format="TEX">\(m\in \left( \frac{q(N+p)}{N},\frac{Np}{N-p}\right) ,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>∈</mo> <mfenced close=")" open="("> <mfrac> <mrow> <mi>q</mi> <mo stretchy="false">(</mo> <mi>N</mi> <mo>+</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> <mi>N</mi> </mfrac> <mo>,</mo> <mfrac> <mrow> <mi mathvariant="italic">Np</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mi>p</mi> </mrow> </mfrac> </mfenced> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> we get the existence of positive ground state normalized solutions for the double phase problem by estimating the energy of the double phase problem and its limit problem and using the Pohozaev constraint.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Normalized Solutions for the Double Phase Problem: Subcritical, Critical and Supercritical Cases

  • Li Cai,
  • Peng Jin

摘要

In this paper, we consider the following double phase problem with combined power nonlinearities and multiple potentials \(\begin{aligned} & -\Delta _p u-\Delta _q u+V(x)(|u|^{p-2}u+|u|^{q-2}u)\\ & \quad =\lambda |u|^{p-2}u+\mu (x)|u|^{m-2}u+|u|^{l-2}u,\quad \text {in}\quad {\mathbb {R}}^N \end{aligned}\) - Δ p u - Δ q u + V ( x ) ( | u | p - 2 u + | u | q - 2 u ) = λ | u | p - 2 u + μ ( x ) | u | m - 2 u + | u | l - 2 u , in R N having prescribed mass \(\begin{aligned} \int _{{\mathbb {R}}^N}|u|^p\,dx=c^p, \end{aligned}\) R N | u | p d x = c p , where \(1<p<q<N,\) 1 < p < q < N , \(p<m<\frac{Np}{N-p},\) p < m < Np N - p , \(\frac{q(N+p)}{N}<l<\frac{Np}{N-p},\) q ( N + p ) N < l < Np N - p , V(x) is an external potential vanishing at infinity, \(\mu (x)\ge 0\) μ ( x ) 0 is a competing potential, and the parameter \(\lambda \in {\mathbb {R}}\) λ R appears as a Lagrange multiplier. Under some mild assumptions on V(x) and \(\mu (x),\) μ ( x ) , for the \(L^p\) L p -subcritical case \(m\in \left( p,\frac{p(N+p)}{N}\right) ,\) m p , p ( N + p ) N , we show that there exists \(c_0>0\) c 0 > 0 such that the normalized solution with negative energy can be obtained when \(c\in (0,c_0)\) c ( 0 , c 0 ) . This is achieved by analyzing the relationship between the energy of double phase problem and its limit problem. For the \(L^p\) L p -critical case \(m=\frac{q(N+p)}{N},\) m = q ( N + p ) N , by limiting the range of parameters, we find the existence of positive ground state normalized solutions with the aid of the Pohozaev constraint and using the properties of the energy in relationship with its limit problem. For the \(L^p\) L p -supercritical case \(m\in \left( \frac{q(N+p)}{N},\frac{Np}{N-p}\right) ,\) m q ( N + p ) N , Np N - p , we get the existence of positive ground state normalized solutions for the double phase problem by estimating the energy of the double phase problem and its limit problem and using the Pohozaev constraint.