<p>In this paper, we consider the following Chern-Simons-Schrödinger system where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_719_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="83" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>u</mi> <mo>∈</mo> <msup> <mi>H</mi> <mn>1</mn> </msup> <mo stretchy="false">(</mo> <msup> <mi mathvariant="double-struck">R</mi> <mn>2</mn> </msup> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$u \in H^{1}(\mathbb{R}^{2})$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_719_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>p</mi> <mo>&gt;</mo> <mn>4</mn> </math></EquationSource> <EquationSource Format="TEX">$p &gt; 4$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_719_Article_IEq3.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="90" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>A</mi> <mi>α</mi> </msub> <mo>:</mo> <msup> <mi mathvariant="double-struck">R</mi> <mn>2</mn> </msup> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">R</mi> </math></EquationSource> <EquationSource Format="TEX">$A_{\alpha }: \mathbb{R}^{2} \rightarrow \mathbb{R}$</EquationSource> </InlineEquation> are the components of the gauge potential, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_719_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="85" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>N</mi> <mo>:</mo> <msup> <mi mathvariant="double-struck">R</mi> <mn>2</mn> </msup> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">R</mi> </math></EquationSource> <EquationSource Format="TEX">$N: \mathbb{R}^{2} \rightarrow \mathbb{R}$</EquationSource> </InlineEquation> is a neutral scalar field, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_719_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="37" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>V</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$V(x)$</EquationSource> </InlineEquation> is a periodic potential function, the parameters <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_719_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>κ</mi> <mo>,</mo> <mi>q</mi> <mo>&gt;</mo> <mn>0</mn> </math></EquationSource> <EquationSource Format="TEX">$\kappa , q&gt;0$</EquationSource> </InlineEquation> represent the Chern-Simons coupling constant and the Maxwell coupling constant, respectively, and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_719_Article_IEq7.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>e</mi> <mo>&gt;</mo> <mn>0</mn> </math></EquationSource> <EquationSource Format="TEX">$e&gt;0$</EquationSource> </InlineEquation> is the coupling constant. We prove that system <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10440_2025_719_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mo stretchy="false">(</mo> <mi>P</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$(P)$</EquationSource> </InlineEquation> has a nontrivial solution by using a new infinite-dimensional linking theorem.</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

Solutions to Strongly Indefinite Chern-Simons-Schrödinger Systems

  • Jin Deng

摘要

In this paper, we consider the following Chern-Simons-Schrödinger system where u H 1 ( R 2 ) $u \in H^{1}(\mathbb{R}^{2})$ , p > 4 $p > 4$ , A α : R 2 R $A_{\alpha }: \mathbb{R}^{2} \rightarrow \mathbb{R}$ are the components of the gauge potential, N : R 2 R $N: \mathbb{R}^{2} \rightarrow \mathbb{R}$ is a neutral scalar field, V ( x ) $V(x)$ is a periodic potential function, the parameters κ , q > 0 $\kappa , q>0$ represent the Chern-Simons coupling constant and the Maxwell coupling constant, respectively, and e > 0 $e>0$ is the coupling constant. We prove that system ( P ) $(P)$ has a nontrivial solution by using a new infinite-dimensional linking theorem.