Abstract

The study of higher order energy functionals was first proposed by Eells and Sampson in 1965 and, later, by Eells and Lemaire in 1983. These functionals provide a natural generalization of the classical energy functional. More precisely, Eells and Sampson suggested the investigation of the so-called $ES-r$-energy functionals $ E_r^{ES}(\varphi) = (1/2)\int_{M}\, |(d^*+d)^r (\varphi)|^2\, dV$, where $r \geq 2 $ and $ \varphi:M \to N$ is a map between two Riemannian manifolds. The initial part of this paper is a short overview on basic definitions, properties, recent developments and open problems concerning the functionals $ E_r^{ES}(\varphi)$ and other, equally interesting, higher order energy functionals $E_r(\varphi)$ which were introduced and studied in various papers by Maeta and other authors. If a critical point $\varphi$ of $E_r^{ES}(\varphi)$ (respectively, $E_r(\varphi)$) is an isometric immersion, then we say that its image is an $ES-r$-harmonic (respectively, $r$-harmonic) submanifold of $N$. We observe that minimal submanifolds are trivially both $ES-r$-harmonic and $r$-harmonic. Therefore, it is natural to say that an $ES-r$-harmonic ($r$-harmonic) submanifold is proper if it is not minimal. In the special case that the ambient space $N$ is the Euclidean space $\mathbb{R}^n$ the notions of $ES-r$-harmonic and $r$-harmonic submanifolds coincide. The Chen-Maeta conjecture is still open: it states that, for all $r \geq2$, any proper, $r$-harmonic submanifold of $\mathbb{R}^n$ is minimal. In the second part of this paper we shall focus on the study of $G = {\rm SO}(p+1) \times {\rm SO}(q+1)$-invariant submanifolds of $\mathbb{R}^n$, $n = p+q+2$. In particular, we shall obtain an explicit description of the relevant Euler-Lagrange equations in the case that $r = 3$ and we shall discuss difficulties and possible developments towards the proof of the Chen-Maeta conjecture for $3$-harmonic $G$-invariant hypersurfaces.

Highlights

  • Harmonic maps are the critical points of the energy functionalE(φ) = 1 |dφ|2 dV, (1.1)where φ : M → N is a smooth map between two Riemannian manifolds (Mm, g) and (Nn, h)

  • Eells and Sampson suggested the investigation of the so-called ES − r-energy functionals ErES (φ) = (1/2) M |(d∗ + d)r(φ)|2 dV, where r ≥ 2 and φ : M → N is a map between two Riemannian manifolds

  • If a critical point φ of ErES (φ) (respectively, Er(φ)) is an isometric immersion, we say that its image is an ES − r-harmonic submanifold of N

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Summary

Introduction

By contrast with the case of Er(φ), the explicit derivation of the Euler-Lagrange equation for the Eells-Sampson functionals ErES (φ) seems, in general, a very complicated task. These difficulties are explained in detail in the recent paper [6], where the Euler-Lagrange equation of the functional E4ES (φ) was computed. To end this introduction, let us briefly point out some of the technical reasons which make the study of the functionals ErES (φ) rather different from that of their companions Er(φ). The leading terms are given by τ4(φ), while τ4(φ) is a differential operator of order 4

The case of space form target
Some geometric applications
Second variation
V0 d ds
Conflict of interest
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