Higher order energy functionals

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 EES (φ) = (1/2) |(d∗ + rM d)r(φ)|2dV, where φ : M → N is a map between two Riemannian manifolds. In the initial part of this paper we shall clarify some relevant issues about the definition of an ES − r-harmonic map, i.e., a critical point of EES (φ). That r seems important to us because in the literature other higher order energy functionals have been studied by several authors and consequently some recent examples need to be discussed and extended: this shall be done in the first two sections of this work, where we obtain the first examples of proper critical points of EES(φ) when N = Sm (r ≥ 4, m ≥ 3), and r we also prove some general facts which should be useful for future developments of this subject. Next, we shall compute the Euler-Lagrange system of equations for EES(φ) for r = 4. We shall apply this result to the study of maps into space forms and to rotationally symmetric maps: in particular, we shall focus on the study of various family of conformal maps. In Section 4, we shall also show that, even if 2r > dim M , the functionals EES(φ) may not satisfy the classical Palais-Smale r Condition (C). In the final part of the paper we shall study the second variation and compute index and nullity of some significant examples.