Lie algebra

In mathematics, a Lie algebra (named after Sophus Lie, pronounced "lee") is an algebraic structure whose main use lies in studying geometric objects such as Lie groups and differentiable manifolds. Lie algebras were introduced to study the concept of infinitesimal transformations.
Contents 
Definition
A Lie algebra is a type of an algebra over a field; it is a vector space g over some field F together with a binary operation [·, ·] : g × g → g, called the Lie bracket, which satisfies the following properties:
 <math> [a x + b y, z] = a [x, z] + b [y, z], \quad [z, a x + b y] = a[z, x] + b [z, y] <math>
 for all a, b ∈ F and all x, y, z ∈ g.
 For all x in g
 <math> [x,x]=0 \quad <math>
 The Jacobi identity:
 <math> [x,[y,z]] + [y,[z,x]] + [z,[x,y]] = 0 \quad <math>
 for all x, y, z in g.
Note that the first and second properties together imply
 <math> [x,y] = [y,x] <math>
for all x, y in g ("antisymmetry"). Conversely, the antisymmetry property implies property 2 above as long as F is not of characteristic 2.
Also note that the multiplication represented by the Lie bracket is not in general associative, that is, <math>[[ x , y ], z ]<math> need not equal <math>[x, [y, z]]<math>. Therefore, Lie algebras are not rings or associative algebras in the usual sense, although much of the same language is used to describe them.
Examples
1. Every vector space becomes an abelian Lie algebra trivially if we define the Lie bracket to be identically zero.
2. Euclidean space R^{3} becomes a Lie algebra with the Lie bracket given by the cross product of vectors.
3. If an associative algebra A with multiplication * is given, it can be turned into a Lie algebra by defining [x, y] = x * y − y * x. This expression is called the commutator of x and y. Conversely, it can be shown that every Lie algebra can be embedded into one that arises from an associative algebra in this fashion. See universal enveloping algebra.
4. Another important example of a Lie algebra comes from differential topology: the smooth vector fields on a differentiable manifold form an infinite dimensional Lie algebra when equipped with the Lie derivative as the Lie bracket. The Lie derivative identifies a vector field X with a partial differential operator acting on any smooth scalar field f by letting X(f) be the directional derivative of f in the direction of X. Then in the expression (YX)(f), the juxtaposition YX represents composition of partial differential operators. Then the Lie bracket [X, Y] is defined by
 [X, Y] f = (XY − YX) f
for every smooth function f on the manifold.
This is the Lie algebra of the infinitedimensional Lie group of diffeomorphisms of the manifold.
5. The vector space of leftinvariant vector fields on a Lie group is closed under this operation and is therefore a finite dimensional Lie algebra. One may alternatively think of the underlying vector space of the Lie algebra belonging to a Lie group as the tangent space at the group's identity element. The multiplication is the differential of the group commutator, (a,b) > aba^{−1}b^{−1}, at the identity element.
6. As a concrete example, consider the Lie group SL(n,R) of all nbyn matrices with real entries and determinant 1. The tangent space at the identity matrix may be identified with the space of all real nbyn matrices with trace 0, and the Lie algebra structure coming from the Lie group coincides with the one arising from commutators of matrix multiplication.
For more examples of Lie groups and their associated Lie algebras, see the Lie group article.
Homomorphisms, subalgebras, and ideals
A homomorphism φ : g → h between Lie algebras g and h over the same base field F is an Flinear map such that [φ(x), φ(y)] = φ([x, y]) for all x and y in g. The composition of such homomorphisms is again a homomorphism, and the Lie algebras over the field F, together with these morphisms, form a category. If such a homomorphism is bijective, it is called an isomorphism, and the two Lie algebras g and h are called isomorphic. For all practical purposes, isomorphic Lie algebras are identical.
A subalgebra of the Lie algebra g is a linear subspace h of g such that [x, y] ∈ h for all x, y ∈ h. The subalgebra is then itself a Lie algebra.
An ideal of the Lie algebra g is a subspace h of g such that [a, y] ∈ h for all a ∈ g and y ∈ h. All ideals are subalgebras. If h is an ideal of g, then the quotient space g/h becomes a Lie algebra by defining [x + h, y + h] = [x, y] + h for all x, y ∈ g. The ideals are precisely the kernels of homomorphisms, and the fundamental theorem on homomorphisms is valid for Lie algebras.
Classification of Lie algebras
Real and complex Lie algebras can be classified to some extent, and this classification is an important step toward the classification of Lie groups. Every finitedimensional real or complex Lie algebra arises as the Lie algebra of unique real or complex simply connected Lie group (Ado's theorem), but there may be more than one group, even more than one connected group, giving rise to the same algebra. For instance, the groups SO(3) (3×3 orthogonal matrices of determinant 1) and SU(2) (2×2 unitary matrices of determinant 1) both give rise to the same Lie algebra, namely R^{3} with crossproduct.
A Lie algebra is abelian if the Lie bracket vanishes, i.e. [x, y] = 0 for all x and y. More generally, a Lie algebra g is nilpotent if the lower central series
 g > [g, g] > [[g, g], g] > [[[g, g], g], g] > ...
becomes zero eventually. By Engel's theorem, a Lie algebra is nilpotent if and only if for every u in g the map
 ad(u): g → g
defined by
 ad(u)(v) = [u,v]
is nilpotent. More generally still, a Lie algebra g is said to be solvable if the derived series
 g > [g, g] > [[g, g], [g,g]] > [[[g, g], [g,g]],[[g, g], [g,g]]] > ...
becomes zero eventually. A maximal solvable subalgebra is called a Borel subalgebra.
A Lie algebra g is called semisimple if the only solvable ideal of g is trivial. Equivalently, g is semisimple if and only if the Killing form K(u,v) = tr(ad(u)ad(v)) is nondegenerate; here tr denotes the trace operator. When the field F is of characteristic zero, g is semisimple if and only if every representation is completely reducible, that is for every invariant subspace of the representation there is an invariant complement (Weyl's theorem).
A Lie algebra is simple if it has no nontrivial ideals and is not abelian. In particular, a simple Lie algebra is semisimple, and more generally, the semisimple Lie algebras are the direct sums of the simple ones.
Semisimple complex Lie algebras are classified through their root systems.
Category theoretic definition
Using the language of category theory, a Lie algebra can be defined as an object A in the category of vector spaces together with a morphism <math>[\cdot,\cdot]:A\otimes A\rightarrow A<math> such that
 <math>[\cdot,\cdot]\circ (id+\tau_{A,A})=0<math>
 <math>[\cdot,\cdot]\circ ([\cdot,\cdot]\otimes id)\circ(id+\sigma+\sigma^2)=0<math>
where σ is the cyclic permutation braiding <math>(id\otimes \tau_{A,A})\circ(\tau_{A,A}\otimes id)<math>. In diagrammatic form:
Liealgebra.png
Image:Liealgebra.png
Related topics
 representation of a Lie algebra
 adjoint representation of a Lie algebra
 Lie superalgebra
 Lie coalgebra
 Lie bialgebra
 Poisson algebra
 anyonic Lie algebra
 Killing form
References
 Humphreys, James E. Introduction to Lie Algebras and Representation Theory, Second printing, revised. Graduate Texts in Mathematics, 9. SpringerVerlag, New York, 1978. ISBN 0387900535
 Jacobson, Nathan, Lie algebras, Republication of the 1962 original. Dover Publications, Inc., New York, 1979. ISBN 0486638324de:LieAlgebra
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