<p>In the present paper, we are concerned with the existence of positive normalized solutions with prescribed&#xa0;<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(L^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>-norm&#xa0;<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\Vert u\Vert _{2}=m\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mo stretchy="false">‖</mo> <mi>u</mi> <mo stretchy="false">‖</mo> </mrow> <mn>2</mn> </msub> <mo>=</mo> <mi>m</mi> </mrow> </math></EquationSource> </InlineEquation> for the following Choquard equations involving a potential <Equation ID="Equ23"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u+V(x)u+\lambda u=(I_{\alpha }*F(u))f(u) &amp; {\textrm{in}}\quad \mathbb {R}^{N},\\ \Vert u\Vert _{2}=m&gt;0, \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <mi>u</mi> <mo>=</mo> <mo stretchy="false">(</mo> <msub> <mi>I</mi> <mi>α</mi> </msub> <mrow /> <mo>∗</mo> <mi>F</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="1em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <msub> <mrow> <mrow /> <mo stretchy="false">‖</mo> <mi>u</mi> <mo stretchy="false">‖</mo> </mrow> <mn>2</mn> </msub> <mo>=</mo> <mi>m</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where&#xa0;<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(N&gt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>&gt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(I_{\alpha }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>I</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation> is the Riesz potential of order&#xa0;<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\alpha \in (0,N)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>N</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. Under assumptions on&#xa0;<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(L^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>-supercritical nonlinearity&#xa0;<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(F'=f\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>F</mi> <mo>′</mo> </msup> <mo>=</mo> <mi>f</mi> </mrow> </math></EquationSource> </InlineEquation>, and&#xa0;<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(V:\mathbb {R}^{N}\rightarrow \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo>:</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(V\leqslant 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo>⩽</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and vanishing at infinity, we show the existence of a positive solution&#xa0;<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\((u,\lambda )\in H^{1}(\mathbb {R}^{N})\times \mathbb {R}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>λ</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mi>H</mi> <mn>1</mn> </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> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> by using a min–max principle.</p>

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Normalized solutions for Choquard equations involving a type of potential

  • Zu Gao,
  • Zhoutian Jiang

摘要

In the present paper, we are concerned with the existence of positive normalized solutions with prescribed  \(L^{2}\) L 2 -norm  \(\Vert u\Vert _{2}=m\) u 2 = m for the following Choquard equations involving a potential \(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u+V(x)u+\lambda u=(I_{\alpha }*F(u))f(u) & {\textrm{in}}\quad \mathbb {R}^{N},\\ \Vert u\Vert _{2}=m>0, \end{array}\right. } \end{aligned}\) - Δ u + V ( x ) u + λ u = ( I α F ( u ) ) f ( u ) in R N , u 2 = m > 0 , where  \(N>2\) N > 2 , \(I_{\alpha }\) I α is the Riesz potential of order  \(\alpha \in (0,N)\) α ( 0 , N ) . Under assumptions on  \(L^2\) L 2 -supercritical nonlinearity  \(F'=f\) F = f , and  \(V:\mathbb {R}^{N}\rightarrow \mathbb {R}\) V : R N R , \(V\leqslant 0\) V 0 , and vanishing at infinity, we show the existence of a positive solution  \((u,\lambda )\in H^{1}(\mathbb {R}^{N})\times \mathbb {R}^{+}\) ( u , λ ) H 1 ( R N ) × R + by using a min–max principle.