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A note on conformal-biharmonic hypersurfaces

Published 4 Feb 2025 in math.DG | (2502.02510v1)

Abstract: The conformal bienergy functional E2<sup>cE_2<sup>c was recently introduced as a modified version of the classical bienergy functional E2E_2 in order to ensure the validity of some conformal invariance properties. The critical points of E2<sup>cE_2<sup>c are called conformal-biharmonic and denoted cc-biharmonic. In this paper we study the cc-biharmonic hypersurfaces M<sup>mM<sup>m with constant principal curvatures in the product space L<sup>m(ε)</sup>×R {\mathbb L}<sup>m(\varepsilon)</sup> \times \mathbb{R} , where L<sup>m(ε)</sup> {\mathbb L}<sup>m(\varepsilon)</sup> denotes a space form of constant sectional curvature ε \varepsilon . Specifically, we demonstrate that M<sup>m</sup> M<sup>m</sup> is either totally geodesic or a cylindrical hypersurface of the form M<sup>m−1</sup>×R M<sup>{m-1}</sup> \times \mathbb{R} , where M<sup>m−1</sup> M<sup>{m-1}</sup> is a cc-biharmonic isoparametric hypersurface in L<sup>m(ε)</sup> {\mathbb L}<sup>m(\varepsilon)</sup> . To provide further insight, we describe the structure of cc-biharmonic isoparametric hypersurfaces in space forms. In the final part, as a preliminary effort to understand cc-biharmonic hypersurfaces M<sup>m</sup> M<sup>m</sup> in L<sup>m(ε)</sup>×R {\mathbb L}<sup>m(\varepsilon)</sup> \times \mathbb{R} with non constant mean curvature, we establish that a totally umbilical cc-biharmonic hypersurface must necessarily be totally geodesic.

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