<p>In this paper we study the following zero mass Schrödinger-Bopp-Podolsky system with critical growth: <Equation ID="Equ38"> <EquationSource Format="TEX">\(\begin{aligned} \begin{array}{ll} \displaystyle \left\{ \begin{array}{ll} \displaystyle -\Delta u+q^2\phi u=\mu |u|^{p-2}u+|u|^{4}u,\quad &amp; x\in \mathbb {R}^3,\\ -\Delta \phi +a^2\Delta ^2\phi =4\pi u^2,\quad &amp; x\in \mathbb {R}^3, \end{array} \right. \end{array} \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <msup> <mi>q</mi> <mn>2</mn> </msup> <mi>ϕ</mi> <mi>u</mi> <mo>=</mo> <msup> <mrow> <mi>μ</mi> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>4</mn> </msup> <mi>u</mi> <mo>,</mo> <mspace width="1em" /> </mrow> </mstyle> </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>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> <mspace width="1em" /> </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> </mstyle> </mtd> </mtr> </mtable> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(a&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(q\ne 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>≠</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <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> is a parameter and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(p\in (3,6)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>3</mn> <mo>,</mo> <mn>6</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. By introducing a new functional framework developed by Caponio et al. [<CitationRef CitationID="CR9">9</CitationRef>], we first establish the existence of positive ground state solutions for the case of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(p\in (3,6)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>3</mn> <mo>,</mo> <mn>6</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. Moreover, for the case of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(p\in (4,6)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>4</mn> <mo>,</mo> <mn>6</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, multiplicity results are obtained by applying an abstract critical point theorem due to Perera [<CitationRef CitationID="CR31">31</CitationRef>].</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Existence and multiplicity results for the zero mass Schrödinger-Bopp-Podolsky system with critical growth

  • Wentao Huang,
  • Li Wang

摘要

In this paper we study the following zero mass Schrödinger-Bopp-Podolsky system with critical growth: \(\begin{aligned} \begin{array}{ll} \displaystyle \left\{ \begin{array}{ll} \displaystyle -\Delta u+q^2\phi u=\mu |u|^{p-2}u+|u|^{4}u,\quad & x\in \mathbb {R}^3,\\ -\Delta \phi +a^2\Delta ^2\phi =4\pi u^2,\quad & x\in \mathbb {R}^3, \end{array} \right. \end{array} \end{aligned}\) - Δ u + q 2 ϕ u = μ | u | p - 2 u + | u | 4 u , x R 3 , - Δ ϕ + a 2 Δ 2 ϕ = 4 π u 2 , x R 3 , where \(a>0\) a > 0 , \(q\ne 0\) q 0 , \(\mu >0\) μ > 0 is a parameter and \(p\in (3,6)\) p ( 3 , 6 ) . By introducing a new functional framework developed by Caponio et al. [9], we first establish the existence of positive ground state solutions for the case of \(p\in (3,6)\) p ( 3 , 6 ) . Moreover, for the case of \(p\in (4,6)\) p ( 4 , 6 ) , multiplicity results are obtained by applying an abstract critical point theorem due to Perera [31].