<p>We consider the existence problem of the following singular Toda system on a compact Riemann surface <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1117_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\((\Sigma , g)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Σ</mi> <mo>,</mo> <mi>g</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> without boundary <Equation ID="Equ75"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1117_Article_Equ75.gif" Format="GIF" Height="85" Rendition="HTML" Resolution="72" Type="Linedraw" Width="499" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta _gu_1=2\overline{\rho }_1\Big ({\frac{h_1e^{u_1}}{\int _{\Sigma }h_1e^{u_1}dV_g}}-1\Big )-\rho _2\Big ({\frac{h_2e^{u_2}}{\int _{\Sigma }h_2e^{u_2}dV_g}}-1\Big )-4\pi \alpha _1(\delta _0-1),\\ \\ -\Delta _gu_2=2\rho _2\big ({\frac{h_2e^{u_2}}{\int _{\Sigma }h_2e^{u_2}dV_g}}-1\big )-\overline{\rho }_1\big ({\frac{h_1e^{u_1}}{\int _{\Sigma }h_1e^{u_1}dV_g}}-1\big )-4\pi \alpha _2(\delta _0-1), \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>g</mi> </msub> <msub> <mi>u</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mover> <mi>ρ</mi> <mo>¯</mo> </mover> <mn>1</mn> </msub> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">(</mo> </mrow> <mfrac> <mrow> <msub> <mi>h</mi> <mn>1</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>1</mn> </msub> </msup> </mrow> <mrow> <msub> <mo>∫</mo> <mi mathvariant="normal">Σ</mi> </msub> <msub> <mi>h</mi> <mn>1</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>1</mn> </msub> </msup> <mi>d</mi> <msub> <mi>V</mi> <mi>g</mi> </msub> </mrow> </mfrac> <mo>-</mo> <mn>1</mn> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">)</mo> </mrow> <mo>-</mo> <msub> <mi>ρ</mi> <mn>2</mn> </msub> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">(</mo> </mrow> <mfrac> <mrow> <msub> <mi>h</mi> <mn>2</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>2</mn> </msub> </msup> </mrow> <mrow> <msub> <mo>∫</mo> <mi mathvariant="normal">Σ</mi> </msub> <msub> <mi>h</mi> <mn>2</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>2</mn> </msub> </msup> <mi>d</mi> <msub> <mi>V</mi> <mi>g</mi> </msub> </mrow> </mfrac> <mo>-</mo> <mn>1</mn> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">)</mo> </mrow> <mo>-</mo> <mn>4</mn> <mi>π</mi> <msub> <mi>α</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi>δ</mi> <mn>0</mn> </msub> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow /> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>g</mi> </msub> <msub> <mi>u</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mi>ρ</mi> <mn>2</mn> </msub> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">(</mo> </mrow> <mfrac> <mrow> <msub> <mi>h</mi> <mn>2</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>2</mn> </msub> </msup> </mrow> <mrow> <msub> <mo>∫</mo> <mi mathvariant="normal">Σ</mi> </msub> <msub> <mi>h</mi> <mn>2</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>2</mn> </msub> </msup> <mi>d</mi> <msub> <mi>V</mi> <mi>g</mi> </msub> </mrow> </mfrac> <mo>-</mo> <mn>1</mn> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">)</mo> </mrow> <mo>-</mo> <msub> <mover> <mi>ρ</mi> <mo>¯</mo> </mover> <mn>1</mn> </msub> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">(</mo> </mrow> <mfrac> <mrow> <msub> <mi>h</mi> <mn>1</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>1</mn> </msub> </msup> </mrow> <mrow> <msub> <mo>∫</mo> <mi mathvariant="normal">Σ</mi> </msub> <msub> <mi>h</mi> <mn>1</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>1</mn> </msub> </msup> <mi>d</mi> <msub> <mi>V</mi> <mi>g</mi> </msub> </mrow> </mfrac> <mo>-</mo> <mn>1</mn> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">)</mo> </mrow> <mo>-</mo> <mn>4</mn> <mi>π</mi> <msub> <mi>α</mi> <mn>2</mn> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi>δ</mi> <mn>0</mn> </msub> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1117_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(h_1,\,h_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>h</mi> <mn>1</mn> </msub> <mo>,</mo> <mspace width="0.166667em" /> <msub> <mi>h</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> are smooth sign-changing functions, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1117_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="274" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\rho }_1:=4\pi (1+\overline{\alpha }_1),\,0&lt;\rho _2&lt;4\pi (1+\overline{\alpha }_2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mover> <mi>ρ</mi> <mo>¯</mo> </mover> <mn>1</mn> </msub> <mo>:</mo> <mo>=</mo> <mn>4</mn> <mi>π</mi> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>+</mo> <msub> <mover> <mi>α</mi> <mo>¯</mo> </mover> <mn>1</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="0.166667em" /> <mn>0</mn> <mo>&lt;</mo> <msub> <mi>ρ</mi> <mn>2</mn> </msub> <mo>&lt;</mo> <mn>4</mn> <mi>π</mi> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>+</mo> <msub> <mover> <mi>α</mi> <mo>¯</mo> </mover> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1117_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="116" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\alpha }_i=\min \{0,\alpha _i\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mover> <mi>α</mi> <mo>¯</mo> </mover> <mi>i</mi> </msub> <mo>=</mo> <mo movablelimits="true">min</mo> <mrow> <mo stretchy="false">{</mo> <mn>0</mn> <mo>,</mo> <msub> <mi>α</mi> <mi>i</mi> </msub> <mo stretchy="false">}</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1117_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha _i&gt;-1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>α</mi> <mi>i</mi> </msub> <mo>&gt;</mo> <mo>-</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1117_Article_IEq6.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="TEX">\(i=1,2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>. Relying on the proof framework developed in&#xa0; [<CitationRef CitationID="CR14">14</CitationRef>], combined with the Pohozaev identity and classical blow-up analysis, we establish existence results under suitable assumptions. Our results generalize the results of Jost and Wang&#xa0; [<CitationRef CitationID="CR18">18</CitationRef>] from regular Toda system with positive weight functions to singular Toda system involving sign-changing weights.</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

Existence Results of Singular Toda Systems with Sign-Changing Weight Functions

  • Qiang Fei

摘要

We consider the existence problem of the following singular Toda system on a compact Riemann surface \((\Sigma , g)\) ( Σ , g ) without boundary \(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta _gu_1=2\overline{\rho }_1\Big ({\frac{h_1e^{u_1}}{\int _{\Sigma }h_1e^{u_1}dV_g}}-1\Big )-\rho _2\Big ({\frac{h_2e^{u_2}}{\int _{\Sigma }h_2e^{u_2}dV_g}}-1\Big )-4\pi \alpha _1(\delta _0-1),\\ \\ -\Delta _gu_2=2\rho _2\big ({\frac{h_2e^{u_2}}{\int _{\Sigma }h_2e^{u_2}dV_g}}-1\big )-\overline{\rho }_1\big ({\frac{h_1e^{u_1}}{\int _{\Sigma }h_1e^{u_1}dV_g}}-1\big )-4\pi \alpha _2(\delta _0-1), \end{array}\right. } \end{aligned}\) - Δ g u 1 = 2 ρ ¯ 1 ( h 1 e u 1 Σ h 1 e u 1 d V g - 1 ) - ρ 2 ( h 2 e u 2 Σ h 2 e u 2 d V g - 1 ) - 4 π α 1 ( δ 0 - 1 ) , - Δ g u 2 = 2 ρ 2 ( h 2 e u 2 Σ h 2 e u 2 d V g - 1 ) - ρ ¯ 1 ( h 1 e u 1 Σ h 1 e u 1 d V g - 1 ) - 4 π α 2 ( δ 0 - 1 ) , where \(h_1,\,h_2\) h 1 , h 2 are smooth sign-changing functions, \(\overline{\rho }_1:=4\pi (1+\overline{\alpha }_1),\,0<\rho _2<4\pi (1+\overline{\alpha }_2)\) ρ ¯ 1 : = 4 π ( 1 + α ¯ 1 ) , 0 < ρ 2 < 4 π ( 1 + α ¯ 2 ) , and \(\overline{\alpha }_i=\min \{0,\alpha _i\}\) α ¯ i = min { 0 , α i } with \(\alpha _i>-1\) α i > - 1 for \(i=1,2\) i = 1 , 2 . Relying on the proof framework developed in  [14], combined with the Pohozaev identity and classical blow-up analysis, we establish existence results under suitable assumptions. Our results generalize the results of Jost and Wang  [18] from regular Toda system with positive weight functions to singular Toda system involving sign-changing weights.