Abstract
Let (M,g) be a three-dimensional steady gradient Ricci soliton which is non-flat and κ-noncollapsed. We prove that (M,g) is isometric to the Bryant soliton up to scaling. This solves a problem mentioned in Perelman’s first paper.
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Acknowledgements
It is a pleasure to thank Professors Huai-Dong Cao, Gerhard Huisken, Sergiu Klainerman, Leon Simon, Brian White, for discussions. The author is grateful to Meng Zhu for comments on an earlier version of this paper.
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The author was supported in part by the National Science Foundation under grants DMS-0905628 and DMS-1201924.
Appendix: The eigenvalues of some elliptic operators on S 2
Appendix: The eigenvalues of some elliptic operators on S 2
In this section, we collect some well-known results concerning the eigenvalues of certain elliptic operators on S 2. In the following, \(g_{S^{2}}\) will denote the standard metric on S 2 with constant Gaussian curvature 1.
Proposition A.1
Let σ be a one-form on S 2 satisfying
where \(\varDelta _{S^{2}}\) denotes the rough Laplacian and μ∈(−∞,1) is a constant. Then σ=0.
Proof
We can find a real-valued function α and a two-form ω such that σ=dα+d ∗ ω. Using the Bochner formula for one-forms, we obtain
Consequently, the function \(\varDelta _{S^{2}} \alpha+ (\mu+1) \alpha\) is constant, and the two-form \(\varDelta _{S^{2}} \omega+ (\mu+1) \omega\) is a constant multiple of the volume form. Since μ+1<2, we conclude that α is constant and ω is a constant multiple of the volume form. Thus, σ=0, as claimed. □
Proposition A.2
Let χ be a symmetric (0,2)-tensor on S 2 satisfying
where \(\overset{\mathrm{o}}{\chi}\) denotes the trace-free part of χ and μ∈(−∞,2) is a constant. Then χ is a constant multiple of \(g_{S^{2}}\).
Proof
The trace of χ satisfies
Since μ<2, we conclude that \(\operatorname {\mathrm {tr}}\chi\) is constant. Moreover, the trace-free part of χ satisfies
Since μ−4<0, it follows that \(\overset{\mathrm{o}}{\chi} = 0\). Putting these facts together, the assertion follows. □
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Brendle, S. Rotational symmetry of self-similar solutions to the Ricci flow. Invent. math. 194, 731–764 (2013). https://doi.org/10.1007/s00222-013-0457-0
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DOI: https://doi.org/10.1007/s00222-013-0457-0