<p>In this paper, we consider the following <i>zero mass</i> Schrödinger–Bopp–Podolsky system: <Equation ID="Equ34"> <EquationSource Format="TEX">\( {\left\{ \begin{array}{ll} -\varDelta u +q^2\phi u=|u|^{p-2}u,\\ -\varDelta \phi +a^2\varDelta ^2\phi =4\pi u^2, \end{array}\right. } {\text { in }} \mathbb {R}^N, \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi>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> <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> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mo>-</mo> <mi>Δ</mi> <mi>ϕ</mi> <mo>+</mo> <msup> <mi>a</mi> <mn>2</mn> </msup> <msup> <mi>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> </mtr> </mtable> </mrow> </mfenced> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> </mrow> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </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> and <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>. We complete the study initiated in [<CitationRef CitationID="CR2">2</CitationRef>], which relied on a perturbation argument to establish the existence of weak solutions. Here, in contrast, our approach, based on the Mountain Pass Theorem and the splitting lemma, directly yields a ground state solution for <InlineEquation ID="IEq3"> <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>. Moreover, by deriving a Pohozaev identity, we further obtain some nonexistence results for suitable <i>p</i>. Finally, based on the minimax characterization, we also analyze, in the radial case, the asymptotic behavior of the solutions obtained as <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(a\rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, thereby establishing a link with the zero mass Schrödinger–Poisson system.</p>

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On a zero mass Schrödinger–Bopp–Podolsky system: ground states, nonexistence results, and asymptotic behavior

  • Alessio Pomponio,
  • Lianfeng Yang

摘要

In this paper, we consider the following zero mass Schrödinger–Bopp–Podolsky system: \( {\left\{ \begin{array}{ll} -\varDelta u +q^2\phi u=|u|^{p-2}u,\\ -\varDelta \phi +a^2\varDelta ^2\phi =4\pi u^2, \end{array}\right. } {\text { in }} \mathbb {R}^N, \) - Δ u + q 2 ϕ u = | u | p - 2 u , - Δ ϕ + a 2 Δ 2 ϕ = 4 π u 2 , in R N , where \(a>0\) a > 0 and \(q\ne 0\) q 0 . We complete the study initiated in [2], which relied on a perturbation argument to establish the existence of weak solutions. Here, in contrast, our approach, based on the Mountain Pass Theorem and the splitting lemma, directly yields a ground state solution for \(p \in (4,6)\) p ( 4 , 6 ) . Moreover, by deriving a Pohozaev identity, we further obtain some nonexistence results for suitable p. Finally, based on the minimax characterization, we also analyze, in the radial case, the asymptotic behavior of the solutions obtained as \(a\rightarrow 0\) a 0 , thereby establishing a link with the zero mass Schrödinger–Poisson system.