<p>In this paper, we deal with the concentration of positive solutions for the fractional Schrödinger-Poisson system involving a logarithmic nonlinearity given in the form <Equation ID="Equ48"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} \varepsilon ^{2s}\left( -\Delta \right) ^{s} u+V(x)u-\phi u= u \log {u^{2}}&amp; \text {in }\mathbb {R}^{3},\\ \varepsilon ^{2t}\left( -\Delta \right) ^{t}\phi =u^{2}&amp; \text {in }\mathbb {R}^{3}, \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msup> <mi>ε</mi> <mrow> <mn>2</mn> <mi>s</mi> </mrow> </msup> <msup> <mfenced close=")" open="("> <mo>-</mo> <mi mathvariant="normal">Δ</mi> </mfenced> <mi>s</mi> </msup> <mi>u</mi> <mo>+</mo> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> <mo>-</mo> <mi>ϕ</mi> <mi>u</mi> <mo>=</mo> <mi>u</mi> <mo>log</mo> <msup> <mi>u</mi> <mn>2</mn> </msup> </mrow> </mtd> <mtd columnalign="left"> <mrow> <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 /> <msup> <mi>ε</mi> <mrow> <mn>2</mn> <mi>t</mi> </mrow> </msup> <msup> <mfenced close=")" open="("> <mo>-</mo> <mi mathvariant="normal">Δ</mi> </mfenced> <mi>t</mi> </msup> <mi>ϕ</mi> <mo>=</mo> <msup> <mi>u</mi> <mn>2</mn> </msup> </mrow> </mtd> <mtd columnalign="left"> <mrow> <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>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\varepsilon &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is a small parameter, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(s, t \in (0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>,</mo> <mi>t</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> satisfy <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(4s+2t &gt; 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>4</mn> <mi>s</mi> <mo>+</mo> <mn>2</mn> <mi>t</mi> <mo>&gt;</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\left( -\Delta \right) ^{\nu }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mfenced close=")" open="("> <mo>-</mo> <mi mathvariant="normal">Δ</mi> </mfenced> <mi>ν</mi> </msup> </math></EquationSource> </InlineEquation>, with <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\nu \in \{s,t\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ν</mi> <mo>∈</mo> <mo stretchy="false">{</mo> <mi>s</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">}</mo> </mrow> </math></EquationSource> </InlineEquation>, is the fractional Laplace operator, and the potential <i>V</i> is continuous satisfying only a local condition. By applying suitable variational arguments, we analyze the existence and concentration behavior of solutions as <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\varepsilon \rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> for the above problem.</p>

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Concentration phenomena for a logarithmic fractional Schrödinger-Poisson system

  • Lin Li,
  • Huo Tao,
  • Patrick Winkert

摘要

In this paper, we deal with the concentration of positive solutions for the fractional Schrödinger-Poisson system involving a logarithmic nonlinearity given in the form \(\begin{aligned} {\left\{ \begin{array}{ll} \varepsilon ^{2s}\left( -\Delta \right) ^{s} u+V(x)u-\phi u= u \log {u^{2}}& \text {in }\mathbb {R}^{3},\\ \varepsilon ^{2t}\left( -\Delta \right) ^{t}\phi =u^{2}& \text {in }\mathbb {R}^{3}, \end{array}\right. } \end{aligned}\) ε 2 s - Δ s u + V ( x ) u - ϕ u = u log u 2 in R 3 , ε 2 t - Δ t ϕ = u 2 in R 3 , where \(\varepsilon >0\) ε > 0 is a small parameter, \(s, t \in (0,1)\) s , t ( 0 , 1 ) satisfy \(4s+2t > 3\) 4 s + 2 t > 3 , \(\left( -\Delta \right) ^{\nu }\) - Δ ν , with \(\nu \in \{s,t\}\) ν { s , t } , is the fractional Laplace operator, and the potential V is continuous satisfying only a local condition. By applying suitable variational arguments, we analyze the existence and concentration behavior of solutions as \(\varepsilon \rightarrow 0\) ε 0 for the above problem.