Sub-Riemannian manifold explained

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)\subsetT(M)

a vector field in

H(M)

is called horizontal. A curve

\gamma

on

M

is called horizontal if
\gamma(t)\in

H\gamma(t)(M)

for any

t

.

A distribution on

H(M)

is called completely non-integrable or bracket generating if for any

x\inM

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),\dotsc\in T_x(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)=

1
inf\int\sqrt{g(
0
\gamma(t),\gamma(t))}

dt,

where infimum is taken along all horizontal curves

\gamma:[0,1]\toM

such that

\gamma(0)=x

,

\gamma(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

\alpha

which describes the orientation of the car. Therefore, the position of the car can be described by a point in a manifold

R2 x 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

R2 x S1.

A closely related example of a sub-Riemannian metric can be constructed on a Heisenberg group: Take two elements

\alpha

and

\beta

in the corresponding Lie algebra such that

\{\alpha,\beta,[\alpha,\beta]\}

spans the entire algebra. The horizontal distribution

H

spanned by left shifts of

\alpha

and

\beta

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