<p>In this paper, we study the following Schrödinger-Newton system <Equation ID="Equ1"> <EquationNumber>0.1</EquationNumber> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} -\Delta u+u=\Phi u, \ &amp; x\in \mathbb {R}^3,\\ -\Delta \Phi =u^2+\rho (x), \ &amp; x\in \mathbb {R}^3, \end{array} \right. \end{aligned}\)</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>u</mi> <mo>=</mo> <mi mathvariant="normal">Φ</mi> <mi>u</mi> <mo>,</mo> <mspace width="4pt" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi mathvariant="normal">Φ</mi> <mo>=</mo> <msup> <mi>u</mi> <mn>2</mn> </msup> <mo>+</mo> <mi>ρ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="4pt" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\rho \in L^{\frac{6}{5}}(\mathbb {R}^3)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ρ</mi> <mo>∈</mo> <msup> <mi>L</mi> <mfrac> <mn>6</mn> <mn>5</mn> </mfrac> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is a doping profile function. The existence and nonexistence results of a ground state solution are established by using variational methods. Interestingly, whether a ground state solution exists is significantly affected by the sign of <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\rho (x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ρ</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. Specifically, we demonstrate that system (<InternalRef RefID="Equ1">0.1</InternalRef>) possesses a positive ground state solution if <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\rho (x)\ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ρ</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Vert \rho \Vert _{L^{\frac{6}{5}}(\mathbb {R}^3)}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">‖</mo> <mi>ρ</mi> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mfrac> <mn>6</mn> <mn>5</mn> </mfrac> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> </math></EquationSource> </InlineEquation> is appropriately small. Conversely, system (<InternalRef RefID="Equ1">0.1</InternalRef>) has no ground state solution if <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\rho (x) \le 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ρ</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo>≤</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. However, by employing a global compactness lemma and a general minimax principle, we succeed in showing that a high energy positive solution exists for system (<InternalRef RefID="Equ1">0.1</InternalRef>) if <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\rho (x) \le 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ρ</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo>≤</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\Vert \rho \Vert _{L^{\frac{6}{5}}(\mathbb {R}^3)}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">‖</mo> <mi>ρ</mi> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mfrac> <mn>6</mn> <mn>5</mn> </mfrac> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> </math></EquationSource> </InlineEquation> is suitably small.</p>

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Existence of positive solution for Schrödinger-Newton system with a doping profile

  • Liying Shan,
  • Wei Shuai,
  • Jianghua Ye

摘要

In this paper, we study the following Schrödinger-Newton system 0.1 \(\begin{aligned} \left\{ \begin{array}{ll} -\Delta u+u=\Phi u, \ & x\in \mathbb {R}^3,\\ -\Delta \Phi =u^2+\rho (x), \ & x\in \mathbb {R}^3, \end{array} \right. \end{aligned}\) - Δ u + u = Φ u , x R 3 , - Δ Φ = u 2 + ρ ( x ) , x R 3 , where \(\rho \in L^{\frac{6}{5}}(\mathbb {R}^3)\) ρ L 6 5 ( R 3 ) is a doping profile function. The existence and nonexistence results of a ground state solution are established by using variational methods. Interestingly, whether a ground state solution exists is significantly affected by the sign of \(\rho (x)\) ρ ( x ) . Specifically, we demonstrate that system (0.1) possesses a positive ground state solution if \(\rho (x)\ge 0\) ρ ( x ) 0 and \(\Vert \rho \Vert _{L^{\frac{6}{5}}(\mathbb {R}^3)}\) ρ L 6 5 ( R 3 ) is appropriately small. Conversely, system (0.1) has no ground state solution if \(\rho (x) \le 0\) ρ ( x ) 0 . However, by employing a global compactness lemma and a general minimax principle, we succeed in showing that a high energy positive solution exists for system (0.1) if \(\rho (x) \le 0\) ρ ( x ) 0 and \(\Vert \rho \Vert _{L^{\frac{6}{5}}(\mathbb {R}^3)}\) ρ L 6 5 ( R 3 ) is suitably small.