<p>Let (<i>M</i>,&#xa0;<i>g</i>) be a compact Riemann surface with area 1. We investigate the Toda system <Equation ID="Equ1"> <EquationNumber>0.1</EquationNumber> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_Equ1.gif" Format="GIF" Height="43" Rendition="HTML" Resolution="72" Type="Linedraw" Width="304" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u_1 = 2\rho _1(h_1e^{u_1}-1) - \rho _2(h_2e^{u_2}-1),\\ -\Delta u_2 = 2\rho _2(h_2e^{u_2}-1) - \rho _1(h_1e^{u_1}-1), \end{array}\right. } \end{aligned}\)</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> <msub> <mi>u</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mi>ρ</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi>h</mi> <mn>1</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>1</mn> </msub> </msup> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <msub> <mi>ρ</mi> <mn>2</mn> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi>h</mi> <mn>2</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>2</mn> </msub> </msup> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <msub> <mi>u</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mi>ρ</mi> <mn>2</mn> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi>h</mi> <mn>2</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>2</mn> </msub> </msup> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <msub> <mi>ρ</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi>h</mi> <mn>1</mn> </msub> <msup> <mi>e</mi> <msub> <mi>u</mi> <mn>1</mn> </msub> </msup> <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>on (<i>M</i>,&#xa0;<i>g</i>) where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="105" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho _1, \rho _2 \in (0,4\pi ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ρ</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>ρ</mi> <mn>2</mn> </msub> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(h_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>h</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(h_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>h</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> are two <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(C^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>C</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> functions on <i>M</i>. When some <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho _i\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ρ</mi> <mi>i</mi> </msub> </math></EquationSource> </InlineEquation> equals <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(4\pi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>4</mn> <mi>π</mi> </mrow> </math></EquationSource> </InlineEquation>, Eq. (<InternalRef RefID="Equ1">0.1</InternalRef>) becomes critical with respect to the Moser-Trudinger inequality for the Toda system, making the existence problem significantly more challenging. In their seminal article (Comm. Pure Appl. Math., 59 (2006), no. 4, 526–558), Jost, Lin, and Wang established sufficient conditions for the existence of solutions to Eq. (<InternalRef RefID="Equ1">0.1</InternalRef>) when <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho _1=4\pi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ρ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>4</mn> <mi>π</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="85" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho _2 \in (0,4\pi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ρ</mi> <mn>2</mn> </msub> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="96" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho _1=\rho _2=4\pi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ρ</mi> <mn>1</mn> </msub> <mo>=</mo> <msub> <mi>ρ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>4</mn> <mi>π</mi> </mrow> </math></EquationSource> </InlineEquation>, assuming that <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(h_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>h</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(h_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>h</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> are both positive. In our previous paper we extended these results to allow <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(h_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>h</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(h_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>h</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> to change signs in the case <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho _1=4\pi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ρ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>4</mn> <mi>π</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="85" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho _2 \in (0,4\pi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ρ</mi> <mn>2</mn> </msub> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. In this paper we further extend the study to prove that Jost-Lin-Wang’s sufficient conditions remain valid even when <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(h_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>h</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(h_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>h</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> can change signs and <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2189_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="96" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho _1=\rho _2=4\pi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ρ</mi> <mn>1</mn> </msub> <mo>=</mo> <msub> <mi>ρ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>4</mn> <mi>π</mi> </mrow> </math></EquationSource> </InlineEquation>. Our proof relies on an improved version of the Moser-Trudinger inequality for the Toda system, along with dedicated analyses similar to Brezis-Merle type and the use of Pohozaev identities.</p>

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Existence Results for Toda Systems With Sign-Changing Prescribed Functions: Part II

  • Linlin Sun,
  • Xiaobao Zhu

摘要

Let (Mg) be a compact Riemann surface with area 1. We investigate the Toda system 0.1 \(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u_1 = 2\rho _1(h_1e^{u_1}-1) - \rho _2(h_2e^{u_2}-1),\\ -\Delta u_2 = 2\rho _2(h_2e^{u_2}-1) - \rho _1(h_1e^{u_1}-1), \end{array}\right. } \end{aligned}\) - Δ u 1 = 2 ρ 1 ( h 1 e u 1 - 1 ) - ρ 2 ( h 2 e u 2 - 1 ) , - Δ u 2 = 2 ρ 2 ( h 2 e u 2 - 1 ) - ρ 1 ( h 1 e u 1 - 1 ) , on (Mg) where \(\rho _1, \rho _2 \in (0,4\pi ]\) ρ 1 , ρ 2 ( 0 , 4 π ] , and \(h_1\) h 1 and \(h_2\) h 2 are two \(C^2\) C 2 functions on M. When some \(\rho _i\) ρ i equals \(4\pi \) 4 π , Eq. (0.1) becomes critical with respect to the Moser-Trudinger inequality for the Toda system, making the existence problem significantly more challenging. In their seminal article (Comm. Pure Appl. Math., 59 (2006), no. 4, 526–558), Jost, Lin, and Wang established sufficient conditions for the existence of solutions to Eq. (0.1) when \(\rho _1=4\pi \) ρ 1 = 4 π , \(\rho _2 \in (0,4\pi )\) ρ 2 ( 0 , 4 π ) or \(\rho _1=\rho _2=4\pi \) ρ 1 = ρ 2 = 4 π , assuming that \(h_1\) h 1 and \(h_2\) h 2 are both positive. In our previous paper we extended these results to allow \(h_1\) h 1 and \(h_2\) h 2 to change signs in the case \(\rho _1=4\pi \) ρ 1 = 4 π , \(\rho _2 \in (0,4\pi )\) ρ 2 ( 0 , 4 π ) . In this paper we further extend the study to prove that Jost-Lin-Wang’s sufficient conditions remain valid even when \(h_1\) h 1 and \(h_2\) h 2 can change signs and \(\rho _1=\rho _2=4\pi \) ρ 1 = ρ 2 = 4 π . Our proof relies on an improved version of the Moser-Trudinger inequality for the Toda system, along with dedicated analyses similar to Brezis-Merle type and the use of Pohozaev identities.