Lie algebra
A Lie algebra over a field k is a vector space
π€ with a bilinear map [,]:π€Γπ€βπ€, called the Lie bracket and denoted (x,y)β¦[x,y]. It is required to satisfy:
-
1.
[x,x]=0 for all xβπ€.
-
2.
The Jacobi identity
: [x,[y,z]]+[y,[z,x]]+[z,[x,y]]=0 for all x,y,zβπ€.
1 Subalgebras & Ideals
A vector subspace π₯ of the Lie algebra π€ is a subalgebra if π₯ is closed under
the Lie bracket operation, or, equivalently, if π₯ itself is a Lie algebra under the same bracket operation as π€. An ideal of π€ is a subspace π₯ for which [x,y]βπ₯ whenever either xβπ₯ or yβπ₯. Note that every ideal is also a subalgebra.
Some general examples of subalgebras:
-
β’
The center of π€, defined by Z(π€):=. It is an ideal of .
-
β’
The normalizer
of a subalgebra is the set . The Jacobi identity guarantees that is always a subalgebra of .
-
β’
The centralizer
of a subset is the set . Again, the Jacobi identity implies that is a subalgebra of .
2 Homomorphisms
Given two Lie algebras and over the field , a homomorphism from to is a linear transformation such that for all . An injective
homomorphism is called a monomorphism
, and a surjective
homomorphism is called an epimorphism
.
The kernel of a homomorphism (considered as a linear transformation) is denoted . It is always an ideal in .
3 Examples
-
β’
Any vector space can be made into a Lie algebra simply by setting for all vectors . The resulting Lie algebra is called an abelian
Lie algebra.
-
β’
If is a Lie group, then the tangent space at the identity
forms a Lie algebra over the real numbers.
-
β’
with the cross product
operation is a nonabelian
three dimensional Lie algebra over .
4 Historical Note
Lie algebras are so-named in honour of Sophus Lie, a Norwegian
mathematician who pioneered the study of these mathematical objects.
Lieβs discovery was tied to his investigation of continuous
transformation groups and symmetries. One joint project with Felix
Klein called for the classification of all finite-dimensional
groups
acting on the plane. The task seemed hopeless owing to the generally
non-linear nature of such group actions
. However, Lie was able to
solve the problem by remarking that a transformation group can be
locally reconstructed from its corresponding βinfinitesimal
generatorsβ, that is to say vector fields corresponding to various
1-parameter subgroups. In terms of this geometric correspondence, the
group composition operation manifests itself as the bracket of vector
fields, and this is very much a linear operation. Thus the task of
classifying group actions in the plane became the task of classifying
all finite-dimensional Lie algebras of planar vector field; a project
that Lie brought to a successful conclusion
.
This βlinearization trickβ proved to be incredibly fruitful and led to great advances in geometry and differential equations. Such advances are based, however, on various results from the theory of Lie algebras. Lie was the first to make significant contributions to this purely algebraic theory, but he was surely not the last.
Title | Lie algebra |
Canonical name | LieAlgebra |
Date of creation | 2013-03-22 12:03:36 |
Last modified on | 2013-03-22 12:03:36 |
Owner | djao (24) |
Last modified by | djao (24) |
Numerical id | 18 |
Author | djao (24) |
Entry type | Definition |
Classification | msc 17B99 |
Related topic | CommutatorBracket |
Related topic | LieGroup |
Related topic | UniversalEnvelopingAlgebra |
Related topic | RootSystem |
Related topic | SimpleAndSemiSimpleLieAlgebras2 |
Defines | Jacobi identity |
Defines | subalgebra |
Defines | ideal |
Defines | normalizer |
Defines | centralizer |
Defines | kernel |
Defines | homomorphism |
Defines | center |
Defines | centre |
Defines | abelian Lie algebra |
Defines | abelian |