<p>In this paper, we consider the existence of normalized positive solutions for the following nonhomogeneous Schrödinger-Poisson-Slater system <Equation ID="Equ60"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{l} - \Delta u + \lambda u + \left( {{{\left| x \right| }^{ - 1}}*{{\left| u \right| }^2}} \right) u = f\left( u \right) + h\left( x \right) ,~u&gt;0,\quad in\;{\mathbb {R}^3},\\ \int _{{\mathbb {R}^3}} {{{\left| u \right| }^2}dx} = m, u \in H^1(\mathbb {R}^3),\\ \end{array} \right. \end{aligned}\)</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>λ</mi> <mi>u</mi> <mo>+</mo> <mfenced close=")" open="("> <mrow> <msup> <mrow> <mfenced close="|" open="|"> <mi>x</mi> </mfenced> </mrow> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mrow /> <mo>∗</mo> <msup> <mrow> <mfenced close="|" open="|"> <mi>u</mi> </mfenced> </mrow> <mn>2</mn> </msup> </mrow> </mfenced> <mi>u</mi> <mo>=</mo> <mi>f</mi> <mfenced close=")" open="("> <mi>u</mi> </mfenced> <mo>+</mo> <mi>h</mi> <mfenced close=")" open="("> <mi>x</mi> </mfenced> <mo>,</mo> <mspace width="3.33333pt" /> <mi>u</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> <mspace width="1em" /> <mi>i</mi> <mi>n</mi> <mspace width="0.277778em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </msub> <mrow> <msup> <mrow> <mfenced close="|" open="|"> <mi>u</mi> </mfenced> </mrow> <mn>2</mn> </msup> <mi>d</mi> <mi>x</mi> </mrow> <mo>=</mo> <mi>m</mi> <mo>,</mo> <mi>u</mi> <mo>∈</mo> <msup> <mi>H</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where the frequency <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> is not fixed and instead appears as a Lagrange multiplier, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(m&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is prescribed, and <i>h</i>(<i>x</i>) is a perturbation. For the case where the nonlinearity <i>f</i> is mass subcritical and purely power-type, we establish the existence of a normalized positive ground state under the assumption that the perturbation <i>h</i>(<i>x</i>) meets certain mild conditions. Conversely, when the nonlinearity <i>f</i> is mass supercritical, we demonstrate the existence of a normalized mountain pass positive solution using variational methods, provided that <i>h</i>(<i>x</i>) is a radially symmetric positive function. This appears to be the first contribution addressing the normalized solutions for such a perturbed equation with a nonlocal term. Our findings may both generalize and enhance some of the recent results found in the literature.</p>

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Normalized positive solutions to nonhomogeneous Schrödinger-Poisson-Slater system

  • Liping Xu,
  • Shuangshuang Qiu

摘要

In this paper, we consider the existence of normalized positive solutions for the following nonhomogeneous Schrödinger-Poisson-Slater system \(\begin{aligned} \left\{ \begin{array}{l} - \Delta u + \lambda u + \left( {{{\left| x \right| }^{ - 1}}*{{\left| u \right| }^2}} \right) u = f\left( u \right) + h\left( x \right) ,~u>0,\quad in\;{\mathbb {R}^3},\\ \int _{{\mathbb {R}^3}} {{{\left| u \right| }^2}dx} = m, u \in H^1(\mathbb {R}^3),\\ \end{array} \right. \end{aligned}\) - Δ u + λ u + x - 1 u 2 u = f u + h x , u > 0 , i n R 3 , R 3 u 2 d x = m , u H 1 ( R 3 ) , where the frequency \(\lambda \) λ is not fixed and instead appears as a Lagrange multiplier, \(m>0\) m > 0 is prescribed, and h(x) is a perturbation. For the case where the nonlinearity f is mass subcritical and purely power-type, we establish the existence of a normalized positive ground state under the assumption that the perturbation h(x) meets certain mild conditions. Conversely, when the nonlinearity f is mass supercritical, we demonstrate the existence of a normalized mountain pass positive solution using variational methods, provided that h(x) is a radially symmetric positive function. This appears to be the first contribution addressing the normalized solutions for such a perturbed equation with a nonlocal term. Our findings may both generalize and enhance some of the recent results found in the literature.