<p>We consider the following Schrödinger-Bopp-Podolsky system with critical and sublinear terms <Equation ID="Equ1"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} - \Delta u+ u+Q(x)\phi u= \vert u\vert ^4 u+ \lambda K(x)\vert u \vert ^{p-1}u&amp; \text{ in } \ \mathbb {R}^3 \\ - \Delta \phi + a^{2}\Delta ^{2} \phi = 4\pi Q(x) u^{2}&amp; \text{ in } \ \mathbb {R}^3. \end{array}\right. } \end{aligned}\)</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> <mi>u</mi> <mo>+</mo> <mi>Q</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>ϕ</mi> <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> <mi>λ</mi> <mi>K</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </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> <mi>Q</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mi>u</mi> <mn>2</mn> </msup> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <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>Here <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(u,\phi :\mathbb {R}^{3}\rightarrow \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>,</mo> <mi>ϕ</mi> <mo>:</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> are the unknowns, <i>Q</i> and <i>K</i> are given functions satisfying mild assumptions, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(a\ge 0, \lambda &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>≥</mo> <mn>0</mn> <mo>,</mo> <mi>λ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> are parameters and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(p\in (0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. We first show existence of infinitely many solutions at negative energy level, including the ground state, when the parameter <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> is small. Then we give general results concerning the structure of the set of solutions. We show also the behaviour of the solutions as the parameters <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(a,\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>,</mo> <mi>λ</mi> </mrow> </math></EquationSource> </InlineEquation> tend to zero. In particular the ground states solutions tends to a ground state solution of the Schrödinger-Poisson system as <i>a</i> tends to zero.</p>

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Schrödinger-Bopp-Podolsky System with Sublinear and Critical Nonlinearities: Solutions at Negative Energy Levels and Asymptotic Behaviour

  • Heydy M. Santos Damian,
  • Gaetano Siciliano

摘要

We consider the following Schrödinger-Bopp-Podolsky system with critical and sublinear terms \(\begin{aligned} {\left\{ \begin{array}{ll} - \Delta u+ u+Q(x)\phi u= \vert u\vert ^4 u+ \lambda K(x)\vert u \vert ^{p-1}u& \text{ in } \ \mathbb {R}^3 \\ - \Delta \phi + a^{2}\Delta ^{2} \phi = 4\pi Q(x) u^{2}& \text{ in } \ \mathbb {R}^3. \end{array}\right. } \end{aligned}\) - Δ u + u + Q ( x ) ϕ u = | u | 4 u + λ K ( x ) | u | p - 1 u in R 3 - Δ ϕ + a 2 Δ 2 ϕ = 4 π Q ( x ) u 2 in R 3 . Here \(u,\phi :\mathbb {R}^{3}\rightarrow \mathbb {R}\) u , ϕ : R 3 R are the unknowns, Q and K are given functions satisfying mild assumptions, \(a\ge 0, \lambda >0\) a 0 , λ > 0 are parameters and \(p\in (0,1)\) p ( 0 , 1 ) . We first show existence of infinitely many solutions at negative energy level, including the ground state, when the parameter \(\lambda \) λ is small. Then we give general results concerning the structure of the set of solutions. We show also the behaviour of the solutions as the parameters \(a,\lambda \) a , λ tend to zero. In particular the ground states solutions tends to a ground state solution of the Schrödinger-Poisson system as a tends to zero.