<p>On a closed Riemannian spin manifold <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="74" /> </InlineMediaObject> <EquationSource Format="TEX">\((M^n,g,\sigma )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msup> <mi>M</mi> <mi>n</mi> </msup> <mo>,</mo> <mi>g</mi> <mo>,</mo> <mi>σ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> with positive scalar curvature we consider the spinorial Yamabe-type equation <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="105" /> </InlineMediaObject> <EquationSource Format="TEX">\(D_g\varphi =\lambda |\varphi |^q\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>D</mi> <mi>g</mi> </msub> <mi>φ</mi> <mo>=</mo> <mi>λ</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>φ</mi> <mo stretchy="false">|</mo> </mrow> <mi>q</mi> </msup> <mi>φ</mi> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation> is a spinor field, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> is a positive constant and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq5.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="82" /> </InlineMediaObject> <EquationSource Format="TEX">\(q\in (0,\frac{2}{n-1}]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mfrac> <mn>2</mn> <mrow> <mi>n</mi> <mo>-</mo> <mn>1</mn> </mrow> </mfrac> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>. For non trivial solutions of this equation we find a positive lower bound for <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda ^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>λ</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>. As an application we obtain a conformal lower bound for the Bär-Hijazi-Lott invariant <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq7.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda _{min}^+\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>λ</mi> <mrow> <mi mathvariant="italic">min</mi> </mrow> <mo>+</mo> </msubsup> </math></EquationSource> </InlineEquation> when <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq8.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(q=\frac{2}{n-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>=</mo> <mfrac> <mn>2</mn> <mrow> <mi>n</mi> <mo>-</mo> <mn>1</mn> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. This estimation allow us to get the classification of solutions for spinorial Yamabe equation <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq9.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="164" /> </InlineMediaObject> <EquationSource Format="TEX">\(D_g\varphi =\lambda _{min}^+|\varphi |^{2/(n-1)}\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>D</mi> <mi>g</mi> </msub> <mi>φ</mi> <mo>=</mo> <msubsup> <mi>λ</mi> <mrow> <mi mathvariant="italic">min</mi> </mrow> <mo>+</mo> </msubsup> <msup> <mrow> <mo stretchy="false">|</mo> <mi>φ</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mn>2</mn> <mo stretchy="false">/</mo> <mo stretchy="false">(</mo> <mi>n</mi> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </msup> <mi>φ</mi> </mrow> </math></EquationSource> </InlineEquation> on manifolds that support a non trivial real Killing spinor. Also we obtain an explicit lower bound for <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda ^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>λ</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> when <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2050_Article_IEq11.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="84" /> </InlineMediaObject> <EquationSource Format="TEX">\(q\in (0,\frac{2}{n-1})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mfrac> <mn>2</mn> <mrow> <mi>n</mi> <mo>-</mo> <mn>1</mn> </mrow> </mfrac> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Spinorial Yamabe-Type Equations and the Bär-Hijazi-Lott Invariant

  • Jurgen Julio-Batalla

摘要

On a closed Riemannian spin manifold \((M^n,g,\sigma )\) ( M n , g , σ ) with positive scalar curvature we consider the spinorial Yamabe-type equation \(D_g\varphi =\lambda |\varphi |^q\varphi \) D g φ = λ | φ | q φ , where \(\varphi \) φ is a spinor field, \(\lambda \) λ is a positive constant and \(q\in (0,\frac{2}{n-1}]\) q ( 0 , 2 n - 1 ] . For non trivial solutions of this equation we find a positive lower bound for \(\lambda ^2\) λ 2 . As an application we obtain a conformal lower bound for the Bär-Hijazi-Lott invariant \(\lambda _{min}^+\) λ min + when \(q=\frac{2}{n-1}\) q = 2 n - 1 . This estimation allow us to get the classification of solutions for spinorial Yamabe equation \(D_g\varphi =\lambda _{min}^+|\varphi |^{2/(n-1)}\varphi \) D g φ = λ min + | φ | 2 / ( n - 1 ) φ on manifolds that support a non trivial real Killing spinor. Also we obtain an explicit lower bound for \(\lambda ^2\) λ 2 when \(q\in (0,\frac{2}{n-1})\) q ( 0 , 2 n - 1 ) .