<p>In this paper, we intend to study the following Schrödinger-Bopp-Podolsky with doubly critical growth in <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {R}^3\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </math></EquationSource> </InlineEquation>: <Equation ID="Equ65"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll}-\Delta u-\phi |u|^{3}u=\lambda u+\mu |u|^{q-2}u+|u|^{4}u &amp; \text{ in } \mathbb {R}^3, \\ -\Delta \phi +a^{2}\Delta ^{2}\phi =4\pi ^{2}|u|^{5}&amp; \text{ in } \mathbb {R}^3, \end{array}\right. } \end{aligned}\)</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> <msup> <mrow> <mi>ϕ</mi> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>3</mn> </msup> <mi>u</mi> <mo>=</mo> <mi>λ</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>q</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> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <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> <msup> <mi>π</mi> <mn>2</mn> </msup> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>5</mn> </msup> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <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>and prescribed mass <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\int _{\mathbb {R}^3} |u|^{2}dx=\varrho ^2,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mi>d</mi> <mi>x</mi> <mo>=</mo> <msup> <mi>ϱ</mi> <mn>2</mn> </msup> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> where <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mu , a, \varrho &gt;0,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>,</mo> <mi>a</mi> <mo>,</mo> <mi>ϱ</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\lambda \in \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(q\in (2, 6)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>2</mn> <mo>,</mo> <mn>6</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. For the <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(L^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>-subcritical case, we show the existence of multiple normalized solutions by using the truncation technique and the genus theory. For the <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(L^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>-supercritical case, we obtain a couple of normalized solutions by developing the auxiliary functional. For both cases, in order to overcome the loss of compactness of the energy functional due to the doubly critical growth, the concentration-compactness principle is needed to overcome this difficulty. As far as we know, this paper is the first attempt that the multiplicity of normalized solutions to the Schrödinger-Bopp-Podolsky system with doubly critical growth. The most obvious and important feature is that we establish some new techniques to prove our results.</p>

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Normalized Solutions for the Schrödinger-Bopp-Podolsky System: Doubly Critical Growth Case

  • Lulu Wei,
  • Yueqiang Song,
  • Sihua Liang

摘要

In this paper, we intend to study the following Schrödinger-Bopp-Podolsky with doubly critical growth in \(\mathbb {R}^3\) R 3 : \(\begin{aligned} {\left\{ \begin{array}{ll}-\Delta u-\phi |u|^{3}u=\lambda u+\mu |u|^{q-2}u+|u|^{4}u & \text{ in } \mathbb {R}^3, \\ -\Delta \phi +a^{2}\Delta ^{2}\phi =4\pi ^{2}|u|^{5}& \text{ in } \mathbb {R}^3, \end{array}\right. } \end{aligned}\) - Δ u - ϕ | u | 3 u = λ u + μ | u | q - 2 u + | u | 4 u in R 3 , - Δ ϕ + a 2 Δ 2 ϕ = 4 π 2 | u | 5 in R 3 , and prescribed mass \(\int _{\mathbb {R}^3} |u|^{2}dx=\varrho ^2,\) R 3 | u | 2 d x = ϱ 2 , where \(\mu , a, \varrho >0,\) μ , a , ϱ > 0 , \(\lambda \in \mathbb {R}\) λ R , \(q\in (2, 6)\) q ( 2 , 6 ) . For the \(L^2\) L 2 -subcritical case, we show the existence of multiple normalized solutions by using the truncation technique and the genus theory. For the \(L^2\) L 2 -supercritical case, we obtain a couple of normalized solutions by developing the auxiliary functional. For both cases, in order to overcome the loss of compactness of the energy functional due to the doubly critical growth, the concentration-compactness principle is needed to overcome this difficulty. As far as we know, this paper is the first attempt that the multiplicity of normalized solutions to the Schrödinger-Bopp-Podolsky system with doubly critical growth. The most obvious and important feature is that we establish some new techniques to prove our results.