Lie Algebras
I am currently learning Lie algebras as they will be really important for my master project. Here are some notes that I have taken about basic notions. I will probably post more stuff about what I am doing later. I am using a program that convert LaTex to WordPress, so I hope it will be readable. Most of the following notions about Lie Algebras were taken in Humphreys’ book. The book has a good basic knowledge in classification of Lie Algebras.
Definition (Lie Algebra)
A vector space
over a field
, with an operation
, denoted
and called the bracket or commutator of
and
, is called a Lie Algebra over
if the following axioms are satisfied:
Bilinearity: The bracket operation is bilinear, i.-e.
,
![{[(ax+by)z] = a[xz] + b[yz]} {[(ax+by)z] = a[xz] + b[yz]}](http://s0.wp.com/latex.php?latex=%7B%5B%28ax%2Bby%29z%5D+%3D+a%5Bxz%5D+%2B+b%5Byz%5D%7D&bg=f0f0f0&fg=000000&s=0)
![{[z(ax+by)] = a[zx]+b[zy]. } {[z(ax+by)] = a[zx]+b[zy]. }](http://s0.wp.com/latex.php?latex=%7B%5Bz%28ax%2Bby%29%5D+%3D+a%5Bzx%5D%2Bb%5Bzy%5D.+%7D&bg=f0f0f0&fg=000000&s=0)
Antisymmetriy:
for all
.
Jacobi identity:
.
Notice that we can deduced from these properties that
.
Definition (Lie Isomorphisms)
We say that two Lie algebras
over
are isomorphic if there exists a vector space isomorphism
satisfying
for all
.
Definition (Lie Subalgebras)
A Lie Subalgebras is a subspace
of
such that
whenever
.
Lie algebras first arose with the study of Lie groups, which are groups that are also smooth manifolds. Lee gives a good introduction in his book to Lie algebras from that point of view.
Let
and
be smooth vector fields on a smooth manifold
. Then the operator
given by:
![\displaystyle [V,W]f = VWf - WVf \displaystyle [V,W]f = VWf - WVf](http://s0.wp.com/latex.php?latex=%5Cdisplaystyle+%5BV%2CW%5Df+%3D+VWf+-+WVf+&bg=f0f0f0&fg=000000&s=0)
is a Lie bracket. It is a smooth vector fields.
Definition (Left-Invariant Vector Fields)
Suppose
is a Lie group. Any
defines maps
, called Left translation and Right translation, respectively, by

A vector field
on
is said to be left-invariant if

The space
of all smooth vector fields on a smooth manifold
is a Lie algebra under the Lie bracket of vector fields. Given
is a Lie group, the set of all smooth left-invariant vector fields on
is a Lie subalgebra of
and is therefore a Lie algebra. It is called the Lie algebra of G and is denoted by
. The reason why this algebra is of particular importance is given by the following theorem:
Theorem
Let
be a Lie group. The evaluation map
, given by
, is a vector space isomorphism. Thus, dim
= dim
.
Let
be a finite dimensional vector space over
, denote by End
the set of linear transformations
. Define the bracket as
. With this operation End
is called the general linear algebra, denoted by
. One interesting theorem links
to
.
Theorem
is isomorphic to
.
Any subalgebra of a Lie algebra
is called a linear Lie algebra.
Some Lie algebras of linear transformations arise most naturally as derivations of algebras. By an F-algebra, we simply mean a vector space
over
endowed with a bilinear operation
. By a derivation of
, we mean a linear map
satisfying the Liebnitz’s rule:
. Let Der
denote the set of all derivations of
. Then, Der
is a subspace of End
. Since the commutator
of two derivations is again a derivation, Der
is a subalgebra of
. Certain derivations arise quite naturally. If
is an endomorphism of
, which is denoted ad
. In fact, ad
Der
. Derivations of this form are called inner and all other are called outer. The map
sending
to ad
is called the adjoint representation of
.
It is know (cf. Jacobson Chapter VI) that every finite dimensional Lie algebra is isomorphic to some linear Lie algebra.
Definition (Abelian Lie algebras)
A Lie algebra is called abelian if
for all
.
1.1. Ideals and homomorphism
A subspace
of a Lie algebra
is called an ideal of
if
,
together imply
.
Example 1 The centre
is an ideal. Another important example of ideal is the derived algebra of
, denoted
, which is analogous to the commutator subgroup of a group. It consists of all linear combinations of commutators
. It is clear that if
are two ideals, then
is an ideal. Similarly,
is an ideal.
If
has no ideals except itself and
, and if moreover
, then
is called a simple Lie algebra.
In the case where
is not simple, and
is a proper ideal of
, then the construction of a quotient algebra is formally the same as the construction of a quotient ring: A quotient space with Lie multiplication defined by
.
The normalizer of a subalgebra (or just subspace)
of
is defined by
. By the Jacobi identity,
is a subalgebra of
. It is the largest subalgebra of
which includes
as an ideal. If
, we call
self-normalizing. The centralizer of a subset
of
is
. It is a subalgebra of
.
A linear transformation
is called an homomorphism if
.
Note that
is an ideal of
. Also, the standard isomorphism theorems hold.
Let
be a vector space over
. A Representation of a Lie algebra
is a homomorphism
.
An important example to bear in mind is the adjoint representation
. The kernel of ad is
. If
is simple, then
, so
is a monomorphism. Then, any simple Lie algebra is isomorphic to a linear Lie algebra.
1.2. Solvable and nilpotent Lie algebras
The derived series of
is defined by
is called solvable if
for some
.
Theorem
Let
be a Lie algebra.
If L is solvable, then so are all subalgebras and homomorphic images of L.
If I is a solvable ideal of
such that
is solvable, then
itself is solvable.
If
are solvable ideals of
, then so is
.
We are now about to define really important Lie algebras. Let
be a maximal solvable ideal of
. Such an ideal exists. Call this ideal the radical of
and denoted Rad
. If
and Rad
, then
is called semisimple. If
is not solvale, i.e.,
Rad
, then
is semisimple.
Define a sequence of ideals of
(the lower central series) by
is called nilpotent if
for some
.
Theorem
Let L be a Lie algebra.
If
is nilpotent, then so are all subalgebras and homomorphic images of
.
If
is nilpotent, then so is
.
If
is nilpotent, then
.
Now if
is any Lie algebra, and
, we call x ad-nilpotent if ad
is a nilpotent endomorphism.
Theorem
All elements of
are ad-nilpotent if and only if
is nilpotent.
James E. Humphreys, Introduction to Lie Algebras and Representation theory, Second Edition, Springer-Verlag, New-York, 1972.
John M. Lee, Introduction to Smooth Manifolds, Springer-Verlag, New-York, 2003.