Abstract

Minimal compact hypersurface in the unit sphere Sn+1 having squared length of shape operator A2<n are totally geodesic and with A2=n are Clifford hypersurfaces. Therefore, classifying totally geodesic hypersurfaces and Clifford hypersurfaces has importance in geometry of compact minimal hypersurfaces in Sn+1. One finds a naturally induced vector field w called the associated vector field and a smooth function ρ called support function on the hypersurface M of Sn+1. It is shown that a necessary and sufficient condition for a minimal compact hypersurface M in S5 to be totally geodesic is that the support function ρ is a non-trivial solution of static perfect fluid equation. Additionally, this result holds for minimal compact hypersurfaces in Sn+1, (n>2), provided the scalar curvature τ is a constant on integral curves of w. Yet other classification of totally geodesic hypersurfaces among minimal compact hypersurfaces in Sn+1 is obtained using the associated vector field w an eigenvector of rough Laplace operator. Finally, a characterization of Clifford hypersurfaces is found using an upper bound on the integral of Ricci curvature in the direction of the vector field Aw.

Highlights

  • It is interesting to note that this differential equation plays an important role in characterizing totally geodesic hypersurfaces in Sn+1 as observed in this paper

  • Let v be the concircular vector field on Sn+1 considered in the introduction, which satisfies Equation (3), where ρ is the function defined on Sn+1 by ρ = Z, N

  • We call w the associated vector field on M and call the functions ρ, f the support function and the associated function, respectively, of M

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Summary

Introduction

Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations. Sn+1 is the totally geodesic sphere Sn. important minimal hypersurfaces of of. It is interesting to note that this differential equation plays an important role in characterizing totally geodesic hypersurfaces in Sn+1 as observed in this paper. As Sn is totally geodesic, for a vector field U on Sn , on using Equation (3), we find U ( f ) = Ug(v, N ) = g(−ρU, N ) = 0, that is, f is a constant c. Corresponding to eigenvector ξ if ∆ξ = −λξ) These raise two questions: (i) Given a minimal compact hypersurface M of Sn+1 that has support function ρ a non-trivial solution of static perfect fluid equation necessarily totally geodesic? Mathematics 2021, 9, 3161 w an eigenvector of the Laplace operator corresponding to eigenvalue 1, is this hypersurface necessarily totally geodesic?

Preliminaries
Characterizations of Totally Geodesic Hypersurfaces
A Characterization of Clifford Hypersurfaces
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