Paper · Feb 25, 2020

Locally constrained curvature flows and geometric inequalities in hyperbolic space

Yingxiang Hu, Haizhong Li, Yong Wei

math.DGWider flowsarXiv:2002.10643v2

As on arXiv

Abstract

In this paper, we first study the locally constrained curvature flow of hypersurfaces in hyperbolic space, which was introduced by Brendle, Guan and Li [7]. This flow preserves the th quermassintegral and decreases th quermassintegral, so the convergence of the flow yields sharp Alexandrov-Fenchel type inequalities in hyperbolic space. Some special cases have been studied in [7]. In the first part of this paper, we show that h-convexity of the hypersurface is preserved along the flow and then the smooth convergence of the flow for h-convex hypersurfaces follows. We then apply this result to establish some new sharp geometric inequalities comparing the integral of th Gauss-Bonnet curvature of a smooth h-convex hypersurface to its th quermassintegral (for ), and comparing the weighted integral of th mean curvature to its th quermassintegral (for ). In particular, we give an affirmative answer to a conjecture proposed by Ge, Wang and Wu in 2015. In the second part of this paper, we introduce a new locally constrained curvature flow using the shifted principal curvatures. This is natural in the context of h-convexity. We prove the smooth convergence to a geodesic sphere of the flow for h-convex hypersurfaces, and provide a new proof of the geometric inequalities proved by Andrews, Chen and the third author of this paper in 2018. We also prove a family of new sharp inequalities involving the weighted integral of th shifted mean curvature for h-convex hypersurfaces, which as application implies a higher order analogue of Brendle, Hung and Wang's [8] inequality.

Submitted
Feb 25, 2020
Last revised
Sep 27, 2020 (v2)
Subjects
math.DG
Journal
Mathematische Annalen, (2022) 382:1425-1474
DOI
10.1007/s00208-020-02076-4

Comments: 38 pages, accepted version for Mathematische Annalen, add Corollary 1.10 to describe the application of the new locally constrained flow (1.11)

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