Abstract
We define a relative entropy for two self-similarly expanding solutions to mean curvature flow of hypersurfaces, asymptotic to the same cone at infinity. Adapting work of White (Indiana Univ Math J 36(3):567–602, 1987) and using recent results of Bernstein (Asymptotic structure of almost eigenfunctions of drift laplacians on conical ends) and Bernstein-Wang (The space of asymptotically conical self-expanders of mean curvature flow), we show that expanders with vanishing relative entropy are unique in a generic sense. This also implies that generically locally entropy minimising expanders are unique.
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Acknowledgements
The authors wish to thank Tom Ilmanen for sharing his ideas. A.D. was supported by the grant ANR-17-CE40-0034 of the French National Research Agency ANR (project CCEM). F.S. was supported by a Leverhulme Trust Research Project Grant RPG-2016-174.
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Communicated by F.C. Marques.
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Appendices
Appendix A. Geometry of normal graphs
Let again \(\Sigma _0,\Sigma _1\) be two expanders asymptotic to the cone \(C(\Gamma )\), and assume \( {\bar{E}}_{1,R_0} = \text {graph}_{{\bar{E}}_{0,R_0}}(u)\) with \(u : {\bar{E}}_{0,R_0} \rightarrow {\mathbb {R}}\). Let \(p \in \Sigma _0\) and choose a local parametrisation F, parametrising an open neighbourhood U of p in \(\Sigma _0\) such that \(F(0)=p\). We can assume that \( g_{ij}=\langle \partial _i F, \partial _j F \rangle \) satisfies
For simplicity we can furthermore assume that the second fundamental form \((h_{ij})\) is diagonalised at p with eigenvalues \(\lambda _1,\ldots , \lambda _n\). A direct calculation, see [10, (2.27)], yields that the normal vector \(\nu _1(q)\), where \(q = p + u(p) \nu _0(q)\), is co-linear to the vector
Denoting the shape operator \(S = (h^i_{\ j})\) we see that thus in coordinate free notation
where \(v:=(1 + |(\text {Id} - uS)^{-1}(\nabla _{\Sigma _0} u)|^2)^{\frac{1}{2}}\). This implies
For the induced metric \({{\tilde{g}}}\) one obtains in the above coordinates at p, again see [10, (2.32)],
which implies
Furthermore, from [10, (2.30)] we have
Since \(H_{\Sigma _1}(p) = {{\tilde{g}}}^{ij}(p) {{\tilde{h}}}_{ij}(p)\) we see that
where \(Q(x,u,\nabla ^{\Sigma _0} u , \nabla _{\Sigma _0}^2 u)\) is quadratic in \(u, \nabla ^{\Sigma _0} u, \nabla _{\Sigma _0}^2u\).
Appendix B. Interpolation inequalities
We recall the following standard interpolation inequalities in multiplicative form.
Lemma B.1
Suppose that \(u \in C^{k}(B_{2})\), then for \(j< k\),
for \(C=C(n,k)\). Similarly, if \(u \in C^{k,\alpha }(B_{2})\), then for \(j+\beta < k+\alpha \),
for \(C=C(n,k,\alpha ,\beta )\).
These follow in a similar manner to the linear inequalities given in [5, Lemma 6.32], except in the proof one should optimize with respect to the parameter \(\mu \) rather than just choosing \(\mu \) sufficiently small. Alternatively, see [6, Lemma A.2].
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Deruelle, A., Schulze, F. Generic uniqueness of expanders with vanishing relative entropy. Math. Ann. 377, 1095–1127 (2020). https://doi.org/10.1007/s00208-020-02004-6
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DOI: https://doi.org/10.1007/s00208-020-02004-6