<p>This paper considers the existence of multiple normalized solutions of the following Schrödinger-Choquard equation <Equation ID="Equ1"> <EquationSource Format="TEX">\(\begin{cases}- \Delta u = \lambda u + k(\varepsilon x)\,(I_{\alpha} * |u|^{q})\,|u|^{q-2}u + \mu (I_{\alpha} * |u|^{p})\,|u|^{p-2}u, \quad x \in \mathbb{R}^N, \\ \displaystyle \int_{\mathbb{R}^N} |u|^2 \, dx = c^2, \qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad x \in \mathbb{R}^N.\end{cases}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mo>{</mo> <mtable columnalign="left left" columnspacing="1em" displaystyle="false" rowspacing=".2em"> <mtr> <mtd> <mo>−</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>=</mo> <mi>λ</mi> <mi>u</mi> <mo>+</mo> <mi>k</mi> <mo stretchy="false">(</mo> <mi>ε</mi> <mi>x</mi> <mo stretchy="false">)</mo> <mspace width="thinmathspace" /> <mo stretchy="false">(</mo> <msub> <mi>I</mi> <mrow> <mi>α</mi> </mrow> </msub> <mo>∗</mo> <mrow> <mo stretchy="false">∣</mo> </mrow> <mi>u</mi> <msup> <mrow> <mo stretchy="false">∣</mo> </mrow> <mrow> <mi>q</mi> </mrow> </msup> <mo stretchy="false">)</mo> <mspace width="thinmathspace" /> <mrow> <mo stretchy="false">∣</mo> </mrow> <mi>u</mi> <msup> <mrow> <mo stretchy="false">∣</mo> </mrow> <mrow> <mi>q</mi> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <mi>μ</mi> <mo stretchy="false">(</mo> <msub> <mi>I</mi> <mrow> <mi>α</mi> </mrow> </msub> <mo>∗</mo> <mrow> <mo stretchy="false">∣</mo> </mrow> <mi>u</mi> <msup> <mrow> <mo stretchy="false">∣</mo> </mrow> <mrow> <mi>p</mi> </mrow> </msup> <mo stretchy="false">)</mo> <mspace width="thinmathspace" /> <mrow> <mo stretchy="false">∣</mo> </mrow> <mi>u</mi> <msup> <mrow> <mo stretchy="false">∣</mo> </mrow> <mrow> <mi>p</mi> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>,</mo> <mspace width="1em" /> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mtd> </mtr> <mtr> <mtd> <mstyle displaystyle="true" scriptlevel="0"> <msub> <mo>∫</mo> <mrow> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </mrow> </msub> <mrow> <mo stretchy="false">∣</mo> </mrow> <mi>u</mi> <msup> <mrow> <mo stretchy="false">∣</mo> </mrow> <mn>2</mn> </msup> <mspace width="thinmathspace" /> <mi>d</mi> <mi>x</mi> <mo>=</mo> <msup> <mi>c</mi> <mn>2</mn> </msup> <mo>,</mo> <mspace width="2em" /> <mspace width="2em" /> <mspace width="2em" /> <mspace width="2em" /> <mspace width="2em" /> <mspace width="2em" /> <mspace width="2em" /> <mspace width="2em" /> <mspace width="2em" /> <mspace width="2em" /> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>.</mo> </mstyle> </mtd> </mtr> </mtable> <mo fence="true" stretchy="true" /> </mrow> </math></EquationSource> </Equation> where <i>c, ε, μ</i> &gt; 0, <i>N</i> ≥ 3, <i>α</i>, ∈ (0; <i>N</i>), <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({{N + \alpha} \over N} &lt; q &lt; 1 + {{\alpha + 2} \over N} &lt; p \le {{N + \alpha } \over {N - 2}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mfrac> <mrow> <mi>N</mi> <mo>+</mo> <mi>α</mi> </mrow> <mi>N</mi> </mfrac> </mrow> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mn>1</mn> <mo>+</mo> <mrow> <mfrac> <mrow> <mi>α</mi> <mo>+</mo> <mn>2</mn> </mrow> <mi>N</mi> </mfrac> </mrow> <mo>&lt;</mo> <mi>p</mi> <mo>≤</mo> <mrow> <mfrac> <mrow> <mi>N</mi> <mo>+</mo> <mi>α</mi> </mrow> <mrow> <mi>N</mi> <mo>−</mo> <mn>2</mn> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, λ ∈ ℝ is a Lagrange multiplier which is unknown, <i>I</i><sub><i>α</i></sub> is the Riesz potential, <i>k</i>:ℝ<sup><i>N</i></sup> → [0; ∞) is a continuous and positive function. When <i>ε</i> is small enough, we prove that the numbers of normalized solutions are at least the numbers of global maximum points of <i>k</i> by Ekeland’s variational principle and truncated skill.</p>

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Existence of Multiple Normalized Solutions for Schrödinger-Choquard Equation with Mixed Nonlinearities

  • Li-qin Tang,
  • Li Wang,
  • Jun Wang

摘要

This paper considers the existence of multiple normalized solutions of the following Schrödinger-Choquard equation \(\begin{cases}- \Delta u = \lambda u + k(\varepsilon x)\,(I_{\alpha} * |u|^{q})\,|u|^{q-2}u + \mu (I_{\alpha} * |u|^{p})\,|u|^{p-2}u, \quad x \in \mathbb{R}^N, \\ \displaystyle \int_{\mathbb{R}^N} |u|^2 \, dx = c^2, \qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad x \in \mathbb{R}^N.\end{cases}\) { Δ u = λ u + k ( ε x ) ( I α u q ) u q 2 u + μ ( I α u p ) u p 2 u , x R N , R N u 2 d x = c 2 , x R N . where c, ε, μ > 0, N ≥ 3, α, ∈ (0; N), \({{N + \alpha} \over N} < q < 1 + {{\alpha + 2} \over N} < p \le {{N + \alpha } \over {N - 2}}\) N + α N < q < 1 + α + 2 N < p N + α N 2 , λ ∈ ℝ is a Lagrange multiplier which is unknown, Iα is the Riesz potential, k:ℝN → [0; ∞) is a continuous and positive function. When ε is small enough, we prove that the numbers of normalized solutions are at least the numbers of global maximum points of k by Ekeland’s variational principle and truncated skill.