Signed zero: Difference between revisions
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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 [[group action|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 (''G'', ''H'') where ''G'' is a [[Lie group]] and ''H'' is a [[closed set|closed]] [[Lie subgroup]] of ''G'' such that the (left) [[coset space]] ''G''/''H'' is [[connected space|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 ''X'' = ''G''/''H'' of a Klein geometry is a [[smooth manifold]] of dimension | |||
:dim ''X'' = dim ''G'' − dim ''H''. | |||
There is a natural smooth [[group action|left action]] of ''G'' on ''X'' given by | |||
:<math>g\cdot(aH) = (ga)H.</math> | |||
Clearly, this action is transitive (take ''a'' = 1), so that one may then regard ''X'' as a [[homogeneous space]] for the action of ''G''. The [[stabilizer (group theory)|stabilizer]] of the identity coset ''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 (''G'', ''H'') by fixing a basepoint ''x''<sub>0</sub> in ''X'' and letting ''H'' be the stabilizer subgroup of ''x''<sub>0</sub> in ''G''. The group ''H'' is necessarily a closed subgroup of ''G'' and ''X'' is naturally [[diffeomorphic]] to ''G''/''H''. | |||
Two Klein geometries (''G''<sub>1</sub>, ''H''<sub>1</sub>) and (''G''<sub>2</sub>, ''H''<sub>2</sub>) are '''geometrically isomorphic''' if there is a [[Lie group isomorphism]] φ : ''G''<sub>1</sub> → ''G''<sub>2</sub> so that φ(''H''<sub>1</sub>) = ''H''<sub>2</sub>. In particular, if φ is [[conjugacy class|conjugation]] by an element ''g'' ∈ ''G'', we see that (''G'', ''H'') and (''G'', ''gHg''<sup>−1</sup>) 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 ''x''<sub>0</sub>). | |||
==Bundle description== | |||
Given a Lie group ''G'' and closed subgroup ''H'', there is natural [[group action|right action]] of ''H'' on ''G'' given by right multiplication. This action is both free and [[proper action|proper]]. The [[orbit (group theory)|orbits]] are simply the left [[coset]]s of ''H'' in ''G''. One concludes that ''G'' has the structure of a smooth [[principal bundle|principal ''H''-bundle]] over the left coset space ''G''/''H'': | |||
:<math>H\to G\to G/H.\,</math> | |||
==Types of Klein geometries== | |||
===Effective geometries=== | |||
The action of ''G'' on ''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 | |||
:<math>K = \{k \in G : g^{-1}kg \in H\;\;\forall g \in G\}.</math> | |||
The kernel ''K'' may also be described as the [[core (group)|core]] of ''H'' in ''G'' (i.e. the largest subgroup of ''H'' that is [[normal subgroup|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 ''K'' = 1 and '''locally effective''' if ''K'' is [[discrete group|discrete]]. If (''G'', ''H'') is a Klein geometry with kernel ''K'', then (''G''/''K'', ''H''/''K'') is an effective Klein geometry canonically associated to (''G'', ''H''). | |||
===Geometrically oriented geometries=== | |||
A Klein geometry (''G'', ''H'') is '''geometrically oriented''' if ''G'' is [[connected space|connected]]. (This does ''not'' imply that ''G''/''H'' is an [[orientability|oriented manifold]]). If ''H'' is connected it follows that ''G'' is also connected (this is because ''G''/''H'' is assumed to be connected, and ''G'' → ''G''/''H'' is a [[fibration]]). | |||
Given any Klein geometry (''G'', ''H''), there is a geometrically oriented geometry canonically associated to (''G'', ''H'') with the same base space ''G''/''H''. This is the geometry (''G''<sub>0</sub>, ''G''<sub>0</sub> ∩ ''H'') where ''G''<sub>0</sub> is the [[identity component]] of ''G''. Note that ''G'' = ''G''<sub>0</sub> ''H''. | |||
===Reductive geometries=== | |||
A Klein geometry (''G'', ''H'') is said to be '''reductive''' and ''G''/''H'' a '''reductive homogeneous space''' if the [[Lie algebra]] <math>\mathfrak h</math> of ''H'' has an ''H''-invariant complement in <math>\mathfrak g</math>. | |||
== 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''' | |||
|- | |||
! ''[[Euclidean geometry]]'' | |||
| [[Euclidean space]] <math>E(n)</math> || [[Euclidean group]] <math>\mathrm{Euc}(n)\simeq \mathrm{O}(n)\rtimes \R^n</math> || [[Orthogonal group]] <math>\mathrm{O}(n)</math> || Distances of [[Euclidean group|points]], [[angle]]s of [[Euclidean vector|vectors]] | |||
|- | |||
! ''[[Spherical geometry]]'' | |||
| [[Sphere]] <math>S^n</math> || Orthogonal group <math>\mathrm{O}(n+1)</math> || Orthogonal group <math>\mathrm{O}(n)</math> || Distances of points, angles of vectors | |||
|- | |||
! ''[[Conformal geometry]] on the sphere'' | |||
| [[Sphere]] <math>S^n</math> || [[Lorentz group]] of an <math>n+2</math> dimensional space <math>\mathrm{O}(n+1,1)</math> || A subgroup <math>P</math> fixing a [[Line (geometry)|line]] in the [[null cone]] of the Minkowski metric || Angles of vectors | |||
|- | |||
! ''[[Projective geometry]]'' | |||
| [[Real projective space]] <math>\mathbb{RP}^n</math> || [[Projective group]] <math>\mathrm{PGL}(n+1)</math>|| A subgroup <math>P</math> fixing a [[Flag (linear algebra)|flag]] <math>\{0\}\subset V_1\subset V_n</math> || [[Projective line]]s, [[Cross-ratio]] | |||
|- | |||
! ''[[Affine geometry]]'' | |||
| [[Affine space]] <math>A(n)\simeq\R^n</math> || [[Affine group]] <math>\mathrm{Aff}(n)\simeq \mathrm{GL}(n)\rtimes \R^n</math> || [[General linear group]] <math>\mathrm{GL}(n)</math> || Lines, Quotient of surface areas of geometric shapes, [[Center of mass]] of [[triangles]]. | |||
|- | |||
! ''[[Hyperbolic geometry]]'' | |||
| [[Hyperbolic space]] <math>H(n)</math>, modeled e.g. as time-like lines in the [[Minkowski space]] <math>\R^{1,n}</math> || Lorentz group <math>\mathrm{O}(1,n)</math> || <math>\mathrm{O}(1)\times \mathrm{O}(n)</math> || Hyperbolic lines, hyperbolic circles, angles. | |||
|- | |||
|} | |||
==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]] |
Revision as of 22:20, 20 January 2014
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 (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 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 a = 1), so that one may then regard X as a homogeneous space for the action of G. The stabilizer of the identity coset 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 (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 (G1, H1) and (G2, H2) are geometrically isomorphic if there is a Lie group isomorphism φ : G1 → G2 so that φ(H1) = H2. In particular, if φ is conjugation by an element g ∈ G, we see that (G, H) and (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 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 K = 1 and locally effective if K is discrete. If (G, H) is a Klein geometry with kernel K, then (G/K, H/K) is an effective Klein geometry canonically associated to (G, H).
Geometrically oriented geometries
A Klein geometry (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 G → G/H is a fibration).
Given any Klein geometry (G, H), there is a geometrically oriented geometry canonically associated to (G, H) with the same base space G/H. This is the geometry (G0, G0 ∩ H) where G0 is the identity component of G. Note that G = G0 H.
Reductive geometries
A Klein geometry (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.
Underlying space | Transformation group G | Subgroup H | Invariants | |
Euclidean geometry | Euclidean space | Euclidean group | Orthogonal group | Distances of points, angles of vectors |
---|---|---|---|---|
Spherical geometry | Sphere | Orthogonal group | Orthogonal group | Distances of points, angles of vectors |
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 | Angles of vectors |
Projective geometry | Real projective space | Projective group | A subgroup fixing a flag | Projective lines, Cross-ratio |
Affine geometry | Affine space | Affine group | General linear group | Lines, Quotient of surface areas of geometric shapes, Center of mass of triangles. |
Hyperbolic geometry | Hyperbolic space , modeled e.g. as time-like lines in the Minkowski space | Lorentz group | Hyperbolic lines, hyperbolic circles, angles. |
References
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