<p>In this paper, we consider the following fractional Schrödinger equation with singular potential and Hartree-type nonlinearity <Equation ID="Equ83"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{l} (-\varDelta )^s u-\frac{u}{|x|^\theta }-\mu |u|^{q-2} u-\eta \left( I_\alpha *h|u|^{2_\alpha }\right) h|u|^{2_\alpha -2} u-\lambda u=0 \; \text{ in } \mathbb {R}^N, \int _{\mathbb {R}^N}u^2 d x=c, \end{array}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi>Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> <mi>u</mi> <mo>-</mo> <mfrac> <mi>u</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mi>θ</mi> </msup> </mfrac> <mo>-</mo> <msup> <mrow> <mi>μ</mi> <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> <mi>η</mi> <mfenced close=")" open="("> <msub> <mi>I</mi> <mi>α</mi> </msub> <mrow /> <mo>∗</mo> <mi>h</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <msub> <mn>2</mn> <mi>α</mi> </msub> </msup> </mfenced> <mi>h</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <msub> <mn>2</mn> <mi>α</mi> </msub> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>-</mo> <mi>λ</mi> <mi>u</mi> <mo>=</mo> <mn>0</mn> <mspace width="0.277778em" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </msub> <msup> <mi>u</mi> <mn>2</mn> </msup> <mi>d</mi> <mi>x</mi> <mo>=</mo> <mi>c</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(s \in \left( \frac{1}{2}, 1\right) , \mu \geqslant 0, c&gt;0, N \geqslant 3,0&lt;\theta &lt;2 s\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>∈</mo> <mfenced close=")" open="("> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mo>,</mo> <mn>1</mn> </mfenced> <mo>,</mo> <mi>μ</mi> <mo>⩾</mo> <mn>0</mn> <mo>,</mo> <mi>c</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> <mi>N</mi> <mo>⩾</mo> <mn>3</mn> <mo>,</mo> <mn>0</mn> <mo>&lt;</mo> <mi>θ</mi> <mo>&lt;</mo> <mn>2</mn> <mi>s</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(2&lt;q&lt;2+\frac{4 s}{N}, 2_\alpha :=\frac{N+\alpha }{N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mn>2</mn> <mo>+</mo> <mfrac> <mrow> <mn>4</mn> <mi>s</mi> </mrow> <mi>N</mi> </mfrac> <mo>,</mo> <msub> <mn>2</mn> <mi>α</mi> </msub> <mo>:</mo> <mo>=</mo> <mfrac> <mrow> <mi>N</mi> <mo>+</mo> <mi>α</mi> </mrow> <mi>N</mi> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\alpha \in (0, N), h: \mathbb {R}^N \rightarrow (0, \infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>N</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mi>h</mi> <mo>:</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo stretchy="false">→</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is a continuous function and <InlineEquation ID="IEq4"> <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> is an unknown Lagrange multiplier. We not only concern with the existence of normalized ground state solutions for the above problem for cases <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mu =\eta =0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>=</mo> <mi>η</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, but also investigate the existence and asymptotic behavior of normalized ground state solutions to the above problem under reasonable assumptions on <i>h</i>(<i>x</i>) for cases <InlineEquation ID="IEq6"> <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> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\eta =1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>η</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Existence and asymptotic behavior of normalized ground state solutions to fractional Schrödinger equation with singular potential and Hartree-type nonlinearity

  • Ding-Wen Zhang,
  • Hong-Rui Sun

摘要

In this paper, we consider the following fractional Schrödinger equation with singular potential and Hartree-type nonlinearity \(\begin{aligned} \left\{ \begin{array}{l} (-\varDelta )^s u-\frac{u}{|x|^\theta }-\mu |u|^{q-2} u-\eta \left( I_\alpha *h|u|^{2_\alpha }\right) h|u|^{2_\alpha -2} u-\lambda u=0 \; \text{ in } \mathbb {R}^N, \int _{\mathbb {R}^N}u^2 d x=c, \end{array}\right. \end{aligned}\) ( - Δ ) s u - u | x | θ - μ | u | q - 2 u - η I α h | u | 2 α h | u | 2 α - 2 u - λ u = 0 in R N , R N u 2 d x = c , where \(s \in \left( \frac{1}{2}, 1\right) , \mu \geqslant 0, c>0, N \geqslant 3,0<\theta <2 s\) s 1 2 , 1 , μ 0 , c > 0 , N 3 , 0 < θ < 2 s , \(2<q<2+\frac{4 s}{N}, 2_\alpha :=\frac{N+\alpha }{N}\) 2 < q < 2 + 4 s N , 2 α : = N + α N , \(\alpha \in (0, N), h: \mathbb {R}^N \rightarrow (0, \infty )\) α ( 0 , N ) , h : R N ( 0 , ) is a continuous function and \(\lambda \in \mathbb {R}\) λ R is an unknown Lagrange multiplier. We not only concern with the existence of normalized ground state solutions for the above problem for cases \(\mu =\eta =0\) μ = η = 0 , but also investigate the existence and asymptotic behavior of normalized ground state solutions to the above problem under reasonable assumptions on h(x) for cases \(\mu >0\) μ > 0 and \(\eta =1\) η = 1 .