<p>Let <i>G</i> = (<i>V</i>,<i>E</i>) be a connected finite graph and Δ be the usual graph Laplacian. In this paper, the authors consider a generalized self-dual Chern-Simons equation on the graph <i>G</i></p><p><Equation ID="Equ1"> <EquationNumber>(0.1)</EquationNumber> <EquationSource Format="TEX">\(\Delta u = - \lambda {{\rm{e}}^{F( u )}}{[ {{{\rm{e}}^{F( u )}} - 1} ]^2} + 4\pi \sum\limits_{j = 1}^M {{\delta _{{p_j}}}},\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>=</mo> <mo>−</mo> <mi>λ</mi> <mrow> <msup> <mrow> <mrow> <mi mathvariant="normal">e</mi> </mrow> </mrow> <mrow> <mi>F</mi> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </msup> </mrow> <mrow> <mo stretchy="false">[</mo> <mrow> <mrow> <msup> <mrow> <mrow> <mi mathvariant="normal">e</mi> </mrow> </mrow> <mrow> <mi>F</mi> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </msup> </mrow> <mo>−</mo> <mn>1</mn> </mrow> <msup> <mo stretchy="false">]</mo> <mn>2</mn> </msup> </mrow> <mo>+</mo> <mn>4</mn> <mi>π</mi> <munderover> <mo movablelimits="false">∑</mo> <mrow> <mi>j</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>M</mi> </munderover> <mrow> <mrow> <msub> <mi>δ</mi> <mrow> <mrow> <msub> <mi>p</mi> <mi>j</mi> </msub> </mrow> </mrow> </msub> </mrow> </mrow> <mo>,</mo> </math></EquationSource> </Equation></p><p>where</p><p><Equation ID="Equa"> <EquationSource Format="TEX">\(F(u) =\begin{cases}{\tilde F\left( u \right)}, &amp; u \le 0,\\0, &amp; u &gt; 0,\end{cases}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>F</mi> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mrow> <mo>{</mo> <mtable> <mtr> <mtd> <mrow> <mrow> <mover> <mi>F</mi> <mo stretchy="false">~</mo> </mover> </mrow> <mrow> <mo>(</mo> <mi>u</mi> <mo>)</mo> </mrow> </mrow> <mo>,</mo> </mtd> <mtd> <mi>u</mi> <mo>≤</mo> <mn>0</mn> <mo>,</mo> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> <mo>,</mo> </mtd> <mtd> <mi>u</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mtd> </mtr> </mtable> <mo fence="true" stretchy="true" /> </mrow> </math></EquationSource> </Equation></p><p><InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\tilde F(u)\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mover> <mi>F</mi> <mo stretchy="false">~</mo> </mover> </mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> satisfies <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(u=1+\tilde F(u)-\rm{{e}}^{\tilde F(u)}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>u</mi> <mo>=</mo> <mn>1</mn> <mo>+</mo> <mrow> <mover> <mi>F</mi> <mo stretchy="false">~</mo> </mover> </mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> <mo>−</mo> <msup> <mrow> <mrow> <mi mathvariant="normal">e</mi> </mrow> </mrow> <mrow> <mrow> <mover> <mi mathvariant="normal">F</mi> <mo stretchy="false">~</mo> </mover> </mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">u</mi> <mo stretchy="false">)</mo> </mrow> </msup> </math></EquationSource> </InlineEquation>, <i>λ</i> &gt; 0, <i>M</i> is any fixed positive integer, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\delta_{p_{j}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mi>δ</mi> <mrow> <msub> <mi>p</mi> <mrow> <mi>j</mi> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> is the Dirac delta mass at the vertex <i>p</i><sub><i>j</i></sub>, and <i>p</i><sub>1</sub>, <i>p</i><sub>2</sub>, …, <i>p</i><sub><i>M</i></sub> are arbitrarily chosen distinct vertices on the graph. They first prove that there is a critical value <i>λ</i><sub><i>c</i></sub> such that if <i>λ</i> ≥ <i>λ</i><sub><i>c</i></sub>, then the generalized self-dual Chern-Simons equation has a solution <i>u</i><sub><i>λ</i></sub>. Applying the existence result, they develop a new method to construct a solution of (0.1) which is monotonic with respect to <i>λ</i> when <i>λ</i> ≥ <i>λ</i><sub><i>c</i></sub>. Then they establish that there exist at least two solutions of the equation for <i>λ</i> &gt; <i>λ</i><sub><i>c</i></sub> via the variational method. Furthermore, they give a fine estimate of the monotone solution, which can be applied to other related problems.</p>

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Existence of Solutions to a Generalized Self-dual Chern-Simons Equation on Graphs

  • Yingshu Lü,
  • Peirong Zhong

摘要

Let G = (V,E) be a connected finite graph and Δ be the usual graph Laplacian. In this paper, the authors consider a generalized self-dual Chern-Simons equation on the graph G

(0.1) \(\Delta u = - \lambda {{\rm{e}}^{F( u )}}{[ {{{\rm{e}}^{F( u )}} - 1} ]^2} + 4\pi \sum\limits_{j = 1}^M {{\delta _{{p_j}}}},\) Δ u = λ e F ( u ) [ e F ( u ) 1 ] 2 + 4 π j = 1 M δ p j ,

where

\(F(u) =\begin{cases}{\tilde F\left( u \right)}, & u \le 0,\\0, & u > 0,\end{cases}\) F ( u ) = { F ~ ( u ) , u 0 , 0 , u > 0 ,

\(\tilde F(u)\) F ~ ( u ) satisfies \(u=1+\tilde F(u)-\rm{{e}}^{\tilde F(u)}\) u = 1 + F ~ ( u ) e F ~ ( u ) , λ > 0, M is any fixed positive integer, \(\delta_{p_{j}}\) δ p j is the Dirac delta mass at the vertex pj, and p1, p2, …, pM are arbitrarily chosen distinct vertices on the graph. They first prove that there is a critical value λc such that if λλc, then the generalized self-dual Chern-Simons equation has a solution uλ. Applying the existence result, they develop a new method to construct a solution of (0.1) which is monotonic with respect to λ when λλc. Then they establish that there exist at least two solutions of the equation for λ > λc via the variational method. Furthermore, they give a fine estimate of the monotone solution, which can be applied to other related problems.