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
:
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|H ∈ X}} 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 : G1 → G2}} so that {{nowrap|1=φ(H1) = H2}}. In particular, if φ is conjugation by an element {{nowrap|g ∈ G}}, 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:
:
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
:
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|G → G/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, G0 ∩ H)}} 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 of H has an H-invariant complement in .
Examples
In the following table, there is a description of the classical geometries, modeled as Klein geometries.
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| Underlying space
| Transformation group G | Subgroup H | Invariants |
Projective geometry
| Real projective space || Projective group || A subgroup fixing a flag || Projective lines, cross-ratio |
---|
Conformal geometry on the sphere
| Sphere || Lorentz group of an -dimensional space || A subgroup fixing a line in the null cone of the Minkowski metric || Generalized circles, angles |
Hyperbolic geometry
| Hyperbolic space , modelled e.g. as time-like lines in the Minkowski space || Orthochronous Lorentz group || || Lines, circles, distances, angles |
Elliptic geometry
| Elliptic space, modelled e.g. as the lines through the origin in Euclidean space || || || Lines, circles, distances, angles |
Spherical geometry
| Sphere || Orthogonal group || Orthogonal group || Lines (great circles), circles, distances of points, angles |
Affine geometry
| Affine space || Affine group || General linear group || Lines, quotient of surface areas of geometric shapes, center of mass of triangles |
Euclidean geometry
| Euclidean space || Euclidean group || Orthogonal group || 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}}