<p>This paper establishes an arbitrary number of solutions for the following Schrödinger–Bopp–Podolsky system with lack of symmetry: <Equation ID="Equ20"> <EquationSource Format="TEX">\( {\left\{ \begin{array}{ll} -\Delta u + V(x) u + \lambda \phi u = f(u), &amp; \text {in}~~ \mathbb {R}^3, \\ -\Delta \phi + a^2\Delta ^2\phi = 4\pi u^2, &amp; \text {in}~~ \mathbb {R}^3, \end{array}\right. } \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>V</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <mi>ϕ</mi> <mi>u</mi> <mo>=</mo> <mi>f</mi> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="3.33333pt" /> <mspace width="3.33333pt" /> <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>ϕ</mi> <mo>+</mo> <msup> <mi>a</mi> <mn>2</mn> </msup> <msup> <mi mathvariant="normal">Δ</mi> <mn>2</mn> </msup> <mi>ϕ</mi> <mo>=</mo> <mn>4</mn> <mi>π</mi> <msup> <mi>u</mi> <mn>2</mn> </msup> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="3.33333pt" /> <mspace width="3.33333pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(a\ne 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>≠</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and the nonlinear function <i>f</i>(<i>t</i>) satisfies the superlinear assumptions only near <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(t=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Using the essential values theory and a new truncation method, we show that for any <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(k \in \mathbb {N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>k</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> </mrow> </math></EquationSource> </InlineEquation>, there exists <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\lambda _k &lt; 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>λ</mi> <mi>k</mi> </msub> <mo>&lt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> such that for all <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\lambda \le \lambda _k\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>≤</mo> <msub> <mi>λ</mi> <mi>k</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, the system admits at least <i>k</i> distinct nontrivial solutions. In this paper, we successfully eliminated the Ambrosetti–Rabinowitz condition, growth conditions at infinity and symmetry condition on the nonlinear function.</p>

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An arbitrary number of solutions for Schrödinger–Bopp–Podolsky systems with lack of symmetry

  • Chen Huang,
  • Chen Dong,
  • Xian Zhang

摘要

This paper establishes an arbitrary number of solutions for the following Schrödinger–Bopp–Podolsky system with lack of symmetry: \( {\left\{ \begin{array}{ll} -\Delta u + V(x) u + \lambda \phi u = f(u), & \text {in}~~ \mathbb {R}^3, \\ -\Delta \phi + a^2\Delta ^2\phi = 4\pi u^2, & \text {in}~~ \mathbb {R}^3, \end{array}\right. } \) - Δ u + V ( x ) u + λ ϕ u = f ( u ) , in R 3 , - Δ ϕ + a 2 Δ 2 ϕ = 4 π u 2 , in R 3 , where \(a\ne 0\) a 0 and the nonlinear function f(t) satisfies the superlinear assumptions only near \(t=0\) t = 0 . Using the essential values theory and a new truncation method, we show that for any \(k \in \mathbb {N}\) k N , there exists \(\lambda _k < 0\) λ k < 0 such that for all \(\lambda \le \lambda _k\) λ λ k , the system admits at least k distinct nontrivial solutions. In this paper, we successfully eliminated the Ambrosetti–Rabinowitz condition, growth conditions at infinity and symmetry condition on the nonlinear function.