Sub-Riemannian geometry, also known as nonholonomic Riemannian geometry or Carnot-Carathodory geometry, represents a rich intersection between differential geometry, control theory, and Lie theory. Unlike Riemannian geometry, where one can move freely in all directions, sub-Riemannian geometry imposes constraints on admissible motions, making the study of distances and curves more complex and interesting.
The Lie group perspective offers powerful tools for understanding sub-Riemannian structures. Many sub-Riemannian manifolds arise naturally from Lie groups, particularly nilpotent Lie groups, where the algebraic properties of the group provide insights into geometric properties of the space.
In the Lie group framework, we consider a connected Lie group G equipped with a sub-Riemannian structure defined by:
The distribution D is said to be bracket-generating if the Lie algebra generated by the vector fields in D spans the entire tangent space at every point. This condition ensures that any two points in the manifold can be connected by curves tangent to D, albeit possibly requiring many changes of direction.
At the heart of sub-Riemannian geometry from the Lie group viewpoint are several key concepts:
A curve : [0,1] G is called horizontal (or admissible) if its derivative '(t) belongs to the distribution D for almost all t [0,1]. Only such curves are permissible in sub-Riemannian motion.
The Carnot-Carathodory distance between points p, q G is defined as:
where L() denotes the length of computed using the metric g. This distance metric defines the geometry of the space, and under reasonable conditions, it induces the same topology as the original manifold.
The exponential map exp: D_p G plays a crucial role in connecting the algebraic and geometrical aspects of the Lie group. For Carnot groups, this map becomes a local diffeomorphism.
Carnot groups form a particularly important class of Lie groups in sub-Riemannian geometry. A Carnot group is a simply connected Lie group whose Lie algebra can be decomposed as a direct sum:
with the property that [V, V] = V_{i+1} for i = 1, ..., k-1 and [V, V] = {0}. The distribution D is typically taken as the left-invariant distribution generated by V.
This layering structure reflects the idea that directions in V represent primary motions, while vectors in V_i for i > 1 represent directions that can only be reached through combinations of motions in lower layers.
The Heisenberg group H is the prototypical example of a Carnot group and serves as a fundamental model for understanding sub-Riemannian geometry. It can be realized as the group of (n+2)(n+2) real matrices of the form:
The Lie algebra of H is generated by the vector fields X_i = _{x_i} - x_i_t for i = 1,...,n and T = _t. These satisfy the commutation relations [X_i, X_j] = 0 for all i,j and [X_i, T] = 0 for all i.
In the Heisenberg group, one can move horizontally along the X_i directions, while the T direction is accessible only through commutations of horizontal moves.
Sub-Riemannian geodesics are the length-minimizing horizontal curves between points. Unlike Riemannian geometry, they are generally not unique and can exhibit complex behaviors.
The study of geodesics in Lie groups benefits greatly from the symmetry properties of the group. For many sub-Riemannian structures on Lie groups, particularly Carnot groups, there exist explicit formulas for geodesics and the distance function.
For the Heisenberg group, the distance between points (x,t) and (x',t') can be expressed using the Carnot-Carathodory metric, which involves solving a transcendental equation in general but has known properties and asymptotics.
Sub-Riemannian geometry, particularly from the Lie group perspective, finds applications in various fields:
Sub-Riemannian geometry from the Lie group viewpoint offers a powerful synthesis of geometric and algebraic approaches to understanding constrained motion. The rich structure of Lie groups provides natural examples and computational tools that have proven invaluable in both theoretical developments and practical applications.
The connection between curvature, geodesics, and the algebraic structure of Lie groups continues to be an active area of research, with implications extending far beyond pure mathematics into physics, engineering, and biology.
