<p>Given a Riemannian submersion <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\((M,g) \rightarrow (B,j)\)</EquationSource> </InlineEquation> each of whose fibers is connected and totally geodesic, we consider a certain 1-parameter family of Riemannian metrics <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\((g_{t})_{t &gt; 0}\)</EquationSource> </InlineEquation> on <i>M</i>, which is called the canonical variation. Let <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\lambda _{1}(g_{t})\)</EquationSource> </InlineEquation> be the first positive eigenvalue of the Laplace–Beltrami operator <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Delta ^{M}_{g_{t}}\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\hbox {Vol}(M,g_{t})\)</EquationSource> </InlineEquation> the volume of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\((M, g_{t})\)</EquationSource> </InlineEquation>. In Bérard-Bergery and Bourguignon (Ill J Math 26(2):181–200,1982 ) showed that the scale-invariant quantity <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\lambda _{1}(g_{t})\hbox {Vol}(M,g_{t})^{2/\hbox {dim}M}\)</EquationSource> </InlineEquation> goes to 0 with <i>t</i>. In this paper, we show that if each fiber is Einstein and (<i>M</i>,&#xa0;<i>g</i>) satisfies a certain condition about its Ricci curvature, then bounds for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\lambda _{1}(g_{t})\)</EquationSource> </InlineEquation> can be obtained. In particular this implies that <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\lambda _{1}(g_{t})\hbox {Vol}(M,g_{t})^{2/\hbox {dim}M}\)</EquationSource> </InlineEquation> goes to <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\infty \)</EquationSource> </InlineEquation> with <i>t</i>. Moreover, using these bounds, we consider stability of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(g_{t}\)</EquationSource> </InlineEquation> as a critical point of the Yamabe functional.</p>

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Remark on Laplacians and Riemannian submersions with totally geodesic fibers

  • Kazumasa Narita

摘要

Given a Riemannian submersion \((M,g) \rightarrow (B,j)\) each of whose fibers is connected and totally geodesic, we consider a certain 1-parameter family of Riemannian metrics \((g_{t})_{t > 0}\) on M, which is called the canonical variation. Let \(\lambda _{1}(g_{t})\) be the first positive eigenvalue of the Laplace–Beltrami operator \(\Delta ^{M}_{g_{t}}\) and \(\hbox {Vol}(M,g_{t})\) the volume of \((M, g_{t})\) . In Bérard-Bergery and Bourguignon (Ill J Math 26(2):181–200,1982 ) showed that the scale-invariant quantity \(\lambda _{1}(g_{t})\hbox {Vol}(M,g_{t})^{2/\hbox {dim}M}\) goes to 0 with t. In this paper, we show that if each fiber is Einstein and (Mg) satisfies a certain condition about its Ricci curvature, then bounds for \(\lambda _{1}(g_{t})\) can be obtained. In particular this implies that \(\lambda _{1}(g_{t})\hbox {Vol}(M,g_{t})^{2/\hbox {dim}M}\) goes to \(\infty \) with t. Moreover, using these bounds, we consider stability of \(g_{t}\) as a critical point of the Yamabe functional.