<p>We are interested in finding prescribed <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>-norm solutions to inhomogeneous nonlinear Schrödinger (INLS) equations. For <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(N\ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>, we treat the equation with combined Hardy–Sobolev power-type nonlinearities <Equation ID="Equ89"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_Equ89.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="432" /> </MediaObject> <EquationSource Format="TEX">\( -\Delta u+\lambda u=\mu |x|^{-b}|u|^{q-2}u+|x|^{-d}|u|^{2^*_{d}-2}u \;\;\text{ in }\;\; \mathbb {R}^N,\, N\ge 3, \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <mi>u</mi> <mo>=</mo> <msup> <mrow> <mi>μ</mi> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mi>b</mi> </mrow> </msup> <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>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mi>d</mi> </mrow> </msup> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <msubsup> <mn>2</mn> <mi>d</mi> <mo>∗</mo> </msubsup> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mspace width="0.277778em" /> <mspace width="0.277778em" /> <mi mathvariant="normal">in</mi> <mspace width="0.277778em" /> <mspace width="0.277778em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi mathvariant="normal">N</mi> </msup> <mo>,</mo> <mspace width="0.166667em" /> <mi mathvariant="normal">N</mi> <mo>≥</mo> <mn>3</mn> <mo>,</mo> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq3.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>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq5.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="86" /> </InlineMediaObject> <EquationSource Format="TEX">\(0&lt;b,d&lt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>b</mi> <mo>,</mo> <mi>d</mi> <mo>&lt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="311" /> </InlineMediaObject> <EquationSource Format="TEX">\(2+(4-2b)/N&lt;q&lt;2+(4-2b)/(N-2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>+</mo> <mo stretchy="false">(</mo> <mn>4</mn> <mo>-</mo> <mn>2</mn> <mi>b</mi> <mo stretchy="false">)</mo> <mo stretchy="false">/</mo> <mi>N</mi> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mn>2</mn> <mo>+</mo> <mo stretchy="false">(</mo> <mn>4</mn> <mo>-</mo> <mn>2</mn> <mi>b</mi> <mo stretchy="false">)</mo> <mo stretchy="false">/</mo> <mo stretchy="false">(</mo> <mi>N</mi> <mo>-</mo> <mn>2</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq7.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="168" /> </InlineMediaObject> <EquationSource Format="TEX">\(2^*_{d}= 2(N-d)/(N-2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mn>2</mn> <mi>d</mi> <mo>∗</mo> </msubsup> <mo>=</mo> <mn>2</mn> <mrow> <mo stretchy="false">(</mo> <mi>N</mi> <mo>-</mo> <mi>d</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">/</mo> <mrow> <mo stretchy="false">(</mo> <mi>N</mi> <mo>-</mo> <mn>2</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is the Hardy–Sobolev critical exponent, while for <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(N=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, we investigate the equation with critical exponential growth <Equation ID="Equ90"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_Equ90.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="235" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \begin{aligned}&amp;-\Delta u+\lambda u=|x|^{-b}f(u) \;\;\text{ in }\;\; \mathbb {R}^2, \end{aligned} \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mtable> <mtr> <mtd /> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <mi>u</mi> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mi>b</mi> </mrow> </msup> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="0.277778em" /> <mspace width="0.277778em" /> <mi mathvariant="normal">in</mi> <mspace width="0.277778em" /> <mspace width="0.277778em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where the nonlinearity <i>f</i>(<i>s</i>) behaves like <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq9.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="TEX">\(\exp (s^2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>exp</mo> <mo stretchy="false">(</mo> <msup> <mi>s</mi> <mn>2</mn> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq10.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="TEX">\(s\rightarrow +\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo stretchy="false">→</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. We extend the existence results due to Alves–Ji–Miyagaki (Calc. Var. 61, 2022) from <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq11.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="69" /> </InlineMediaObject> <EquationSource Format="TEX">\(b =d= 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>b</mi> <mo>=</mo> <mi>d</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> to the case <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11784_2025_1228_Article_IEq12.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="86" /> </InlineMediaObject> <EquationSource Format="TEX">\(0&lt; b,d &lt; 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>b</mi> <mo>,</mo> <mi>d</mi> <mo>&lt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Normalized solutions for INLS equation with critical Hardy–Sobolev type nonlinearities

  • M. Cardoso,
  • J. F. de Oliveira,
  • O. H. Miyagaki

摘要

We are interested in finding prescribed \(L^2\) L 2 -norm solutions to inhomogeneous nonlinear Schrödinger (INLS) equations. For \(N\ge 3\) N 3 , we treat the equation with combined Hardy–Sobolev power-type nonlinearities \( -\Delta u+\lambda u=\mu |x|^{-b}|u|^{q-2}u+|x|^{-d}|u|^{2^*_{d}-2}u \;\;\text{ in }\;\; \mathbb {R}^N,\, N\ge 3, \) - Δ u + λ u = μ | x | - b | u | q - 2 u + | x | - d | u | 2 d - 2 u in R N , N 3 , where \(\lambda \in \mathbb {R}\) λ R , \(\mu >0\) μ > 0 , \(0<b,d<2\) 0 < b , d < 2 , \(2+(4-2b)/N<q<2+(4-2b)/(N-2)\) 2 + ( 4 - 2 b ) / N < q < 2 + ( 4 - 2 b ) / ( N - 2 ) and \(2^*_{d}= 2(N-d)/(N-2)\) 2 d = 2 ( N - d ) / ( N - 2 ) is the Hardy–Sobolev critical exponent, while for \(N=2\) N = 2 , we investigate the equation with critical exponential growth \(\begin{aligned} \begin{aligned}&-\Delta u+\lambda u=|x|^{-b}f(u) \;\;\text{ in }\;\; \mathbb {R}^2, \end{aligned} \end{aligned}\) - Δ u + λ u = | x | - b f ( u ) in R 2 , where the nonlinearity f(s) behaves like \(\exp (s^2)\) exp ( s 2 ) as \(s\rightarrow +\infty \) s + . We extend the existence results due to Alves–Ji–Miyagaki (Calc. Var. 61, 2022) from \(b =d= 0\) b = d = 0 to the case \(0< b,d < 2\) 0 < b , d < 2 .