Sub-Riemannian manifold

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Short description: Type of generalization of a Riemannian manifold

In mathematics, a sub-Riemannian manifold is a certain type of generalization of a Riemannian manifold. Roughly speaking, to measure distances in a sub-Riemannian manifold, you are allowed to go only along curves tangent to so-called horizontal subspaces.

Sub-Riemannian manifolds (and so, a fortiori, Riemannian manifolds) carry a natural intrinsic metric called the metric of Carnot–Carathéodory. The Hausdorff dimension of such metric spaces is always an integer and larger than its topological dimension (unless it is actually a Riemannian manifold).

Sub-Riemannian manifolds often occur in the study of constrained systems in classical mechanics, such as the motion of vehicles on a surface, the motion of robot arms, and the orbital dynamics of satellites. Geometric quantities such as the Berry phase may be understood in the language of sub-Riemannian geometry. The Heisenberg group, important to quantum mechanics, carries a natural sub-Riemannian structure.

Definitions

By a distribution on M we mean a subbundle of the tangent bundle of M (see also distribution).

Given a distribution H(M)T(M) a vector field in H(M) is called horizontal. A curve γ on M is called horizontal if γ˙(t)Hγ(t)(M) for any t.

A distribution on H(M) is called completely non-integrable or bracket generating if for any xM we have that any tangent vector can be presented as a linear combination of Lie brackets of horizontal fields, i.e. vectors of the form A(x), [A,B](x), [A,[B,C]](x), [A,[B,[C,D]]](x),Tx(M) where all vector fields A,B,C,D, are horizontal. This requirement is also known as Hörmander's condition.

A sub-Riemannian manifold is a triple (M,H,g), where M is a differentiable manifold, H is a completely non-integrable "horizontal" distribution and g is a smooth section of positive-definite quadratic forms on H.

Any (connected) sub-Riemannian manifold carries a natural intrinsic metric, called the metric of Carnot–Carathéodory, defined as

d(x,y)=inf01g(γ˙(t),γ˙(t))dt,

where infimum is taken along all horizontal curves γ:[0,1]M such that γ(0)=x, γ(1)=y. Horizontal curves can be taken either Lipschitz continuous, Absolutely continuous or in the Sobolev space H1([0,1],M) producing the same metric in all cases.

The fact that the distance of two points is always finite (i.e. any two points are connected by an horizontal curve) is a consequence of Hörmander's condition known as Chow–Rashevskii theorem.

Examples

A position of a car on the plane is determined by three parameters: two coordinates x and y for the location and an angle α which describes the orientation of the car. Therefore, the position of the car can be described by a point in a manifold

2×S1.

One can ask, what is the minimal distance one should drive to get from one position to another? This defines a Carnot–Carathéodory metric on the manifold

2×S1.

A closely related example of a sub-Riemannian metric can be constructed on a Heisenberg group: Take two elements α and β in the corresponding Lie algebra such that

{α,β,[α,β]}

spans the entire algebra. The horizontal distribution H spanned by left shifts of α and β is completely non-integrable. Then choosing any smooth positive quadratic form on H gives a sub-Riemannian metric on the group.

Properties

For every sub-Riemannian manifold, there exists a Hamiltonian, called the sub-Riemannian Hamiltonian, constructed out of the metric for the manifold. Conversely, every such quadratic Hamiltonian induces a sub-Riemannian manifold.

Solutions of the corresponding Hamilton–Jacobi equations for the sub-Riemannian Hamiltonian are called geodesics, and generalize Riemannian geodesics.

See also

References