Klein geometry

{{Short description|Type of geometry}}

In mathematics, a Klein geometry is a type of geometry motivated by Felix Klein in his influential Erlangen program. More specifically, it is a homogeneous space X together with a transitive action on X by a Lie group G, which acts as the symmetry group of the geometry.

For background and motivation see the article on the Erlangen program.

Formal definition

A Klein geometry is a pair {{nowrap|(G, H)}} where G is a Lie group and H is a closed Lie subgroup of G such that the (left) coset space G/H is connected. The group G is called the principal group of the geometry and G/H is called the space of the geometry (or, by an abuse of terminology, simply the Klein geometry). The space {{nowrap|1=X = G/H}} of a Klein geometry is a smooth manifold of dimension

:dim X = dim G − dim H.

There is a natural smooth left action of G on X given by

:g \cdot (aH) = (ga)H.

Clearly, this action is transitive (take {{nowrap|1=a = 1}}), so that one may then regard X as a homogeneous space for the action of G. The stabilizer of the identity coset {{nowrap|HX}} is precisely the group H.

Given any connected smooth manifold X and a smooth transitive action by a Lie group G on X, we can construct an associated Klein geometry {{nowrap|(G, H)}} by fixing a basepoint x0 in X and letting H be the stabilizer subgroup of x0 in G. The group H is necessarily a closed subgroup of G and X is naturally diffeomorphic to G/H.

Two Klein geometries {{nowrap|(G1, H1)}} and {{nowrap|(G2, H2)}} are geometrically isomorphic if there is a Lie group isomorphism {{nowrap|φ : G1G2}} so that {{nowrap|1=φ(H1) = H2}}. In particular, if φ is conjugation by an element {{nowrap|gG}}, we see that {{nowrap|(G, H)}} and {{nowrap|(G, gHg−1)}} are isomorphic. The Klein geometry associated to a homogeneous space X is then unique up to isomorphism (i.e. it is independent of the chosen basepoint x0).

Bundle description

Given a Lie group G and closed subgroup H, there is natural right action of H on G given by right multiplication. This action is both free and proper. The orbits are simply the left cosets of H in G. One concludes that G has the structure of a smooth principal H-bundle over the left coset space G/H:

:H\to G\to G/H .

Types of Klein geometries

=Effective geometries=

The action of G on {{nowrap|1=X = G/H}} need not be effective. The kernel of a Klein geometry is defined to be the kernel of the action of G on X. It is given by

:K = \{k \in G : g^{-1}kg \in H\;\;\forall g \in G\}.

The kernel K may also be described as the core of H in G (i.e. the largest subgroup of H that is normal in G). It is the group generated by all the normal subgroups of G that lie in H.

A Klein geometry is said to be effective if {{nowrap|1=K = 1}} and locally effective if K is discrete. If {{nowrap|(G, H)}} is a Klein geometry with kernel K, then {{nowrap|(G/K, H/K)}} is an effective Klein geometry canonically associated to {{nowrap|(G, H)}}.

=Geometrically oriented geometries=

A Klein geometry {{nowrap|(G, H)}} is geometrically oriented if G is connected. (This does not imply that G/H is an oriented manifold). If H is connected it follows that G is also connected (this is because G/H is assumed to be connected, and {{nowrap|GG/H}} is a fibration).

Given any Klein geometry {{nowrap|(G, H)}}, there is a geometrically oriented geometry canonically associated to {{nowrap|(G, H)}} with the same base space G/H. This is the geometry {{nowrap|(G0, G0H)}} where G0 is the identity component of G. Note that {{nowrap|1=G = G0 H}}.

=Reductive geometries=

A Klein geometry {{nowrap|(G, H)}} is said to be reductive and G/H a reductive homogeneous space if the Lie algebra \mathfrak h of H has an H-invariant complement in \mathfrak g.

Examples

In the following table, there is a description of the classical geometries, modeled as Klein geometries.

class="wikitable" border="1"; text-align:center; margin:.5em 0 .5em 1em;"
| Underlying space

| Transformation group G

| Subgroup H

| Invariants

Projective geometry

| Real projective space \mathbb{R}\mathrm{P}^n || Projective group \mathrm{PGL}(n+1)|| A subgroup P fixing a flag \{0\}\subset V_1\subset V_n || Projective lines, cross-ratio

Conformal geometry on the sphere

| Sphere S^n || Lorentz group of an (n+2)-dimensional space \mathrm{O}(n+1,1) || A subgroup P fixing a line in the null cone of the Minkowski metric || Generalized circles, angles

Hyperbolic geometry

| Hyperbolic space H(n), modelled e.g. as time-like lines in the Minkowski space \R^{1,n} || Orthochronous Lorentz group \mathrm{O}(1,n)/\mathrm{O}(1) || \mathrm{O}(1)\times \mathrm{O}(n) || Lines, circles, distances, angles

Elliptic geometry

| Elliptic space, modelled e.g. as the lines through the origin in Euclidean space \mathbb{R}^{n+1} || \mathrm{O}(n+1)/\mathrm{O}(1) || \mathrm{O}(n)/\mathrm{O}(1) || Lines, circles, distances, angles

Spherical geometry

| Sphere S^n || Orthogonal group \mathrm{O}(n+1) || Orthogonal group \mathrm{O}(n) || Lines (great circles), circles, distances of points, angles

Affine geometry

| Affine space A(n)\simeq\R^n || Affine group \mathrm{Aff}(n)\simeq \R^n \rtimes \mathrm{GL}(n) || General linear group \mathrm{GL}(n) || Lines, quotient of surface areas of geometric shapes, center of mass of triangles

Euclidean geometry

| Euclidean space E(n) || Euclidean group \mathrm{Euc}(n)\simeq \R^n \rtimes \mathrm{O}(n) || Orthogonal group \mathrm{O}(n) || Distances of points, angles of vectors, areas

References

  • {{cite book | author=R. W. Sharpe | title=Differential Geometry: Cartan's Generalization of Klein's Erlangen Program | publisher=Springer-Verlag | year=1997 | isbn=0-387-94732-9}}

Category:Differential geometry

Category:Lie groups

Category:Homogeneous spaces