Vector field cycles in the tangent bundle
Abstract
Given a closed Riemannian manifold (Mm,g) and a vector field v on M, we form the Sasaki metric gS on TM, and restrict it to the image of the cross section map of M into TM defined by v, whose pull back to M defines a new metric g(v) on M. We then view the cross section as an isometric embedding fg(v): (M,g(v))→ (TM,gS), which when \| v\|g=1, ranges into the unit sphere bundle (S1(TM),gS). v is minimal or minimal unit if these embeddings have null mean curvature vectors, conditions that occur if, v is in the kernel or is an eigenvector, respectively, of a first order perturbation of a weighted rough Laplacian, the weights and perturbation determined by the covariant derivatives ∇gev along unit directions e in suitable normal frames that include v when \| v\|g=1, and curvature tensor of g. A minimal unit field must be Killing, and other than parallel fields, v=0 is the only minimal one. We characterize the minimal unit vector fields on the standard sphere (S2n+1,g) (R2n+2,\| \, \|2) as those defining contact strictly pseudoconvex CR structures whose Levi form and sign are determined by g and the orientation. If fg(v)(M) and fg(v)(M) are the total exterior scalar curvature and squared L2 norm of the mean curvature vector functionals, and m>2, a canonical cycle fg(v)(M) is a critical point of the functional (m/m-1) fg(v)(M) +fg(v)(M) under conformal deformations, notion conveniently defined also when m≤ 2. The zero section of TM is a canonical cycle if, and only if, the scalar curvature of g is constant. We describe some examples of these vector fields and cycles, and analyze their deformations under dilations of the field.
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