<p>In this paper, we classify the solutions to the Liouville equation with Neumann boundary on the unit disc <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\overline{\mathbb {B}^2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mn>2</mn> </msup> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation> as follows <Equation ID="Equ45"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u=e^{2u},&amp; \text{ in } {\mathbb {B}^2},\\ \frac{\partial u}{\partial \nu }+\lambda =0 ,&amp; \text{ on } {\mathbb {S}^{1}}, \end{array}\right. } \end{aligned}\)</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> <msup> <mi>e</mi> <mrow> <mn>2</mn> <mi>u</mi> </mrow> </msup> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mn>2</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mfrac> <mrow> <mi>∂</mi> <mi>u</mi> </mrow> <mrow> <mi>∂</mi> <mi>ν</mi> </mrow> </mfrac> <mo>+</mo> <mi>λ</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>on</mtext> <mspace width="0.333333em" /> <msup> <mrow> <mi mathvariant="double-struck">S</mi> </mrow> <mn>1</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\lambda \in \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\nu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ν</mi> </math></EquationSource> </InlineEquation> is the outer unit normal on <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathbb {S}^{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">S</mi> </mrow> <mn>1</mn> </msup> </math></EquationSource> </InlineEquation>. The equation is related to an Onofri-type inequality with Neumann boundary on <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathbb {B}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>. Employing some important integral identities with the Obata identity, we prove the classification results to the above equation for <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(0&lt;\lambda \le 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>λ</mi> <mo>≤</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Classification of Solutions to the Liouville Equation with Neumann Boundary on the Unit Disc

  • Jingbo Dou,
  • Lulu Xu

摘要

In this paper, we classify the solutions to the Liouville equation with Neumann boundary on the unit disc \(\overline{\mathbb {B}^2}\) B 2 ¯ as follows \(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u=e^{2u},& \text{ in } {\mathbb {B}^2},\\ \frac{\partial u}{\partial \nu }+\lambda =0 ,& \text{ on } {\mathbb {S}^{1}}, \end{array}\right. } \end{aligned}\) - Δ u = e 2 u , in B 2 , u ν + λ = 0 , on S 1 , where \(\lambda \in \mathbb {R}\) λ R , \(\nu \) ν is the outer unit normal on \(\mathbb {S}^{1}\) S 1 . The equation is related to an Onofri-type inequality with Neumann boundary on \(\mathbb {B}^2\) B 2 . Employing some important integral identities with the Obata identity, we prove the classification results to the above equation for \(0<\lambda \le 1\) 0 < λ 1 .