The weighted conformal mean curvature flow

We introduce a Yamabe-type flow$ R^m_{\phi} = 0 \; \; \mbox{ in } M \; \; \mbox{ and }\; \; \left\{ \begin{array}{ll} \frac{\partial g}{\partial t} & = 2(h^m_{\phi}-H^m_{\phi})g \\ \frac{\partial \phi}{\partial t} & = m(H^m_{\phi}-h^m_{\phi}) \end{array} \right. \; \; \mbox{ on } \partial M $on a smooth metric measure space with boundary $ (M, g, e^{-\phi}dV_g, e^{-\phi}dA_g, m) $, where $ R^m_{\phi} $ is the weighted scalar curvature, $ H^m_{\phi} $ is the weighted mean curvature and $ h^m_{\phi} $ is the average of the weighted mean curvature. We prove the long-time existence and convergence of this flow.

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Publication Details

Journal
Discrete and Continuous Dynamical Systems
Published
2024-12-12
DOI
https://doi.org/10.3934/dcds.2024171
Citations
1
Primary Topic
Geometric Analysis and Curvature Flows
Type
article
Field-Weighted Citation Impact
0.97
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article

The weighted conformal mean curvature flow

Pak Tung Ho, Zetian Yan, Jinwoo Shin
1 citations
Discrete and Continuous Dynamical Systems
Geometric Analysis and Curvature Flows
0.97
article

The weighted conformal mean curvature flow

Pak Tung Ho, Zetian Yan, Jinwoo Shin
article en
1 citations

Abstract

We introduce a Yamabe-type flow$ R^m_{\phi} = 0 \; \; \mbox{ in } M \; \; \mbox{ and }\; \; \left\{ \begin{array}{ll} \frac{\partial g}{\partial t} & = 2(h^m_{\phi}-H^m_{\phi})g \\ \frac{\partial \phi}{\partial t} & = m(H^m_{\phi}-h^m_{\phi}) \end{array} \right. \; \; \mbox{ on } \partial M $on a smooth metric measure space with boundary $ (M, g, e^{-\phi}dV_g, e^{-\phi}dA_g, m) $, where $ R^m_{\phi} $ is the weighted scalar curvature, $ H^m_{\phi} $ is the weighted mean curvature and $ h^m_{\phi} $ is the average of the weighted mean curvature. We prove the long-time existence and convergence of this flow.

Discrete and Continuous Dynamical SystemsVol. 45(8)
University of California, Santa Barbara (US), Sookmyung Women's University (KR)
Climate action
Openalex Percentile: Top 22%
Geometric Analysis and Curvature Flows
0.97
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