Spectral analysis and geometry of a sub-Riemannian structure on and (original) (raw)

Modified action and differential operators on the 3-D sub-Riemannian sphere

2008

Our main aim is to present a geometrically meaningful formula for the fundamental solutions to a second order sub-elliptic differential equation and to the heat equation associated with a sub-elliptic operator in the sub-Riemannian geometry on the unit sphere mathbbS3\mathbb S^3mathbbS3. Our method is based on the Hamiltonian approach, where the corresponding Hamitonian system is solved with mixed boundary conditions. A closed form of the modified action is given. It is a sub-Riemannian invariant and plays the role of a distance on mathbbS3\mathbb S^3mathbbS3.

Sub-Riemannian Geodesics on the 3-D Sphere

Complex Analysis and Operator Theory, 2009

The unit sphere S 3 can be identified with the unitary group SU (2). Under this identification the unit sphere can be considered as a non-commutative Lie group. The commutation relations for the vector fields of the corresponding Lie algebra define a 2-step sub-Riemannian manifold. We study sub-Riemannian geodesics on this sub-Riemannian manifold making use of the Hamiltonian formalism and solving the corresponding Hamiltonian system.

The Geometry of Sub-Riemannian Three-Manifolds

2003

The local equivalence problem for sub-Riemannian structures on threemanifolds is solved. In the course of the solution, it is shown how to attach a canonical Riemannian metric and connection to the given sub-Riemannian metric and it is shown how all of the differential invariants of the sub-Riemannian structure can be calculated. The relation between the completeness of the sub-Riemannian metric, the associated Riemannian metric, and geodesic completeness is investigated, and an example is given of a manifold that is complete in the sub-Riemannian metric but not complete in the canonical associated Riemannian metric. It is shown that the Jacobi equations for subRiemannian geodesics can be interpreted as a scalar, fourth-order, self-adjoint linear operator along each geodesic. The influence of the differential invariants of the subRiemannian structure on the conjugate points is investigated, and the results are used to prove a Bonnet-Myers-type theorem for complete sub-Riemannian 3-m...

On the second variation of the spectral zeta function of the Laplacian on homogeneous Riemanniann manifolds

Loughborough University, 2014

The spectral zeta function, introduced by Minakshisundaram and Pleijel in [36] and denoted by ζ g (s), encodes important spectral information for the Laplacian on Riemannian manifolds. For instance, the important notions of the determinant of the Laplacian and Casimir energy are defined via the spectral zeta function. On homogeneous manifolds, it is known that the spectral zeta function is critical with respect to conformal metric perturbations, (see e.g Richardson ([47]) and Okikiolu ([41])). In this thesis, we compute a second variation formula of ζ g (s) on closed homogeneous Riemannian manifolds under conformal metric perturbations. It is well known that the quadratic form corresponding to this second variation is given by a certain pseudodifferential operator that depends meromorphically on s. The symbol of this operator was analysed by Okikiolu in ([42]). We analyse it in more detail on homogeneous spaces, in particular on the spheres S n. The case n = 3 is treated in great detail. In order to describe the second variation we introduce a certain distributional integral kernel, analyse its meromorphic properties and the pole structure. The Casimir energy defined as the finite part of ζ g (− 1 2) on the n-sphere and other points of ζ g (s) are used to illustrate our results. The techniques employed are heat kernel asymptotics on Riemannian manifolds, the associated meromorphic continuation of the zeta function, harmonic analysis on spheres, and asymptotic analysis. vi

SubRiemannian geometry on the sphere mathbbS3\mathbb{S}^3mathbbS3

2008

The present paper starts with an introduction to quaternions and then defines the 3-dimmensional sphere as the set of quaternions of length one. The quaternion group induces on mathbbS3\mathbb{S}^3mathbbS3 a structure of noncommutative Lie group. This group is compact and the results obtained in this case are very different than those obtained in the case of the Heisenberg group, which is a noncompact Lie group. Like in the Heisenberg group case, we introduce a nonintegrable distribution on the sphere and a metric on it using two of the noncommutative left invariant vector fields. This way mathbbS3\mathbb{S}^3mathbbS3 becomes a subRiemannian manifold. It is known that the group SU(2)SU(2) SU(2) is isomorphic with the sphere mathbbS3\mathbb{S}^3mathbbS3 and represents an example of subRiemannian manifold where the elements are matrices. The main issue here is to study the connectivity by horizontal curves and its geodesics on this manifold. In this paper, we are using Lagrangian method to study the connectivity theorem on ${\mathbb ...

SubRiemannian geometry on the sphere S^3

2008

The present paper starts with an introduction to quaternions and then defines the 3-dimmensional sphere as the set of quaternions of length one. The quaternion group induces on S^3 a structure of noncommutative Lie group. This group is compact and the results obtained in this case are very different than those obtained in the case of the Heisenberg group, which is a noncompact Lie group. Like in the Heisenberg group case, we introduce a nonintegrable distribution on the sphere and a metric on it using two of the noncommutative left invariant vector fields. This way S^3 becomes a subRiemannian manifold. It is known that the group SU(2) is isomorphic with the sphere S^3 and represents an example of subRiemannian manifold where the elements are matrices. The main issue here is to study the connectivity by horizontal curves and its geodesics on this manifold. In this paper, we are using Lagrangian method to study the connectivity theorem on S^3 by horizontal curves with minimal arc-leng...