In physics, Lie groups appear as symmetry groups of physical systems, and their Lie algebras (tangent vectors near the identity) may be thought of as infinitesimal symmetry motions. Thus Lie algebras and their representations are used extensively in physics, notably in quantum mechanics and particle physics.
An elementary example is the space of three dimensional vectors with the bracket operation defined by the cross product This is skew-symmetric since , and instead of associativity it satisfies the Jacobi identity:
This is the Lie algebra of the Lie group of rotations of space, and each vector may be pictured as an infinitesimal rotation around the axis , with velocity equal to the magnitude of . The Lie bracket is a measure of the non-commutativity between two rotations: since a rotation commutes with itself, we have the alternating property .
for all elements , in . If the field's characteristic is not 2 then anticommutativity implies alternativity, since it implies 
It is customary to denote a Lie algebra by a lower-case fraktur letter such as . If a Lie algebra is associated with a Lie group, then the algebra is denoted by the fraktur version of the group: for example the Lie algebra of SU(n) is .
Generators and dimension
Elements of a Lie algebra are said to generate it if the smallest subalgebra containing these elements is itself. The dimension of a Lie algebra is its dimension as a vector space over . The cardinality of a minimal generating set of a Lie algebra is always less than or equal to its dimension.
The Lie bracket is not required to be associative, meaning that need not equal . However, it is flexible. Nonetheless, much of the terminology of associative rings and algebras is commonly applied to Lie algebras. A Lie subalgebra is a subspace which is closed under the Lie bracket. An ideal is a subalgebra satisfying the stronger condition:
A Lie algebra homomorphism is a linear map compatible with the respective Lie brackets:
As for associative rings, ideals are precisely the kernels of homomorphisms; given a Lie algebra and an ideal in it, one constructs the factor algebra or quotient algebra, and the first isomorphism theorem holds for Lie algebras.
Since the Lie bracket is a kind of infinitesimal commutator of the corresponding Lie group, we say that two elements commute if their bracket vanishes: .
The centralizer subalgebra of a subset is the set of elements commuting with : that is, . The centralizer of itself is the center. Similarly, for a subspace S, the normalizer subalgebra of is . Equivalently, if is a Lie subalgebra, is the largest subalgebra such that is an ideal of .
For , the commutator of two elements and :
shows is a subalgebra, but not an ideal. In fact, every one-dimensional linear subspace of a Lie algebra has an induced abelian Lie algebra structure, which is generally not an ideal. For any simple Lie algebra, all abelian Lie algebras can never be ideals.
Direct sum and semidirect product
For two Lie algebras and , their direct sum Lie algebra is the vector space consisting of all pairs , with the operation
for all . The inner derivation associated to any is the adjoint mapping defined by . (This is a derivation as a consequence of the Jacobi identity.) The outer derivations are derivations which do not come from the adjoint representation of the Lie algebra. If is semisimple, every derivation is inner.
The derivations form a vector space , which is a Lie subalgebra of ; the bracket is commutator. The inner derivations form a Lie subalgebra of .
For example, given a Lie algebra ideal the adjoint representation of acts as outer derivations on since for any and . For the Lie algebra of upper triangular matrices in , it has an ideal of strictly upper triangular matrices (where the only non-zero elements are above the diagonal of the matrix). For instance, the commutator of elements in and gives
shows there exist outer derivations from in .
Split Lie algebra
Let V be a finite-dimensional vector space over a field F, the Lie algebra of linear transformations and a Lie subalgebra. Then is said to be split if the roots of the characteristic polynomials of all linear transformations in are in the base field F. More generally, a finite-dimensional Lie algebra is said to be split if it has a Cartan subalgebra whose image under the adjoint representation is a split Lie algebra. A split real form of a complex semisimple Lie algebra (cf. #Real form and complexification) is an example of a split real Lie algebra. See also split Lie algebra for further information.
Vector space basis
For practical calculations, it is often convenient to choose an explicit vector space basis for the algebra. A common construction for this basis is sketched in the article structure constants.
Definition using category-theoretic notation
Although the definitions above are sufficient for a conventional understanding of Lie algebras, once this is understood, additional insight can be gained by using notation common to category theory, that is, by defining a Lie algebra in terms of linear maps—that is, morphisms of the category of vector spaces—without considering individual elements. (In this section, the field over which the algebra is defined is supposed to be of characteristic different from two.)
For the category-theoretic definition of Lie algebras, two braiding isomorphisms are needed. If A is a vector space, the interchange isomorphism is defined by
The cyclic-permutation braiding is defined as
where is the identity morphism.
Equivalently, is defined by
With this notation, a Lie algebra can be defined as an object in the category of vector spaces together with a morphism
that satisfies the two morphism equalities
Any vector space endowed with the identically zero Lie bracket becomes a Lie algebra. Such Lie algebras are called abelian, cf. below. Any one-dimensional Lie algebra over a field is abelian, by the alternating property of the Lie bracket.
Associative algebra with commutator bracket
On an associative algebra over a field with multiplication , a Lie bracket may be defined by the commutator. With this bracket, is a Lie algebra. The associative algebra A is called an enveloping algebra of the Lie algebra . Every Lie algebra can be embedded into one that arises from an associative algebra in this fashion; see universal enveloping algebra.
For a finite dimensional vector space , the previous example is exactly the Lie algebra of n × n matrices, denoted or , and with bracket where adjacency indicates matrix multiplication. This is the Lie algebra of the general linear group, consisting of invertible matrices.
A complex matrix group is a Lie group consisting of matrices, , where the multiplication of G is matrix multiplication. The corresponding Lie algebra is the space of matrices which are tangent vectors to G inside the linear space : this consists of derivatives of smooth curves in G at the identity:
The Lie bracket of is given by the commutator of matrices, . Given the Lie algebra, one can recover the Lie group as the image of the matrix exponential mapping defined by , which converges for every matrix : that is, .
The following are examples of Lie algebras of matrix Lie groups:
The special linear group, consisting of all n × n matrices with determinant 1. Its Lie algebra consists of all n × n matrices with complex entries and trace 0. Similarly, one can define the corresponding real Lie group and its Lie algebra .
The unitary group consists of n × n unitary matrices (satisfying ). Its Lie algebra consists of skew-self-adjoint matrices ().
The special orthogonal group, consisting of real determinant-one orthogonal matrices (). Its Lie algebra consists of real skew-symmetric matrices (). The full orthogonal group , without the determinant-one condition, consists of and a separate connected component, so it has the same Lie algebra as . See also infinitesimal rotations with skew-symmetric matrices. Similarly, one can define a complex version of this group and algebra, simply by allowing complex matrix entries.
On any field there is, up to isomorphism, a single two-dimensional nonabelian Lie algebra. With generators x, y, its bracket is defined as . It generates the affine group in one dimension.
This can be realized by the matrices:
for any natural number and any , one sees that the resulting Lie group elements are upper triangular 2×2 matrices with unit lower diagonal:
The Heisenberg algebra is a three-dimensional Lie algebra generated by elements x, y, and z with Lie brackets
It is usually realized as the space of 3×3 strictly upper-triangular matrices, with the commutator Lie bracket and the basis
An important class of infinite-dimensional real Lie algebras arises in differential topology. The space of smooth vector fields on a differentiable manifoldM forms a Lie algebra, where the Lie bracket is defined to be the commutator of vector fields. One way of expressing the Lie bracket is through the formalism of Lie derivatives, which identifies a vector field X with a first order partial differential operator LX acting on smooth functions by letting LX(f) be the directional derivative of the function f in the direction of X. The Lie bracket [X,Y] of two vector fields is the vector field defined through its action on functions by the formula:
Kac–Moody algebras are a large class of infinite-dimensional Lie algebras whose structure is very similar to the finite-dimensional cases above.
One important aspect of the study of Lie algebras (especially semisimple Lie algebras) is the study of their representations. (Indeed, most of the books listed in the references section devote a substantial fraction of their pages to representation theory.) Although Ado's theorem is an important result, the primary goal of representation theory is not to find a faithful representation of a given Lie algebra . Indeed, in the semisimple case, the adjoint representation is already faithful. Rather the goal is to understand all possible representation of , up to the natural notion of equivalence. In the semisimple case over a field of characteristic zero, Weyl's theorem says that every finite-dimensional representation is a direct sum of irreducible representations (those with no nontrivial invariant subspaces). The irreducible representations, in turn, are classified by a theorem of the highest weight.
Representation theory in physics
The representation theory of Lie algebras plays an important role in various parts of theoretical physics. There, one considers operators on the space of states that satisfy certain natural commutation relations. These commutation relations typically come from a symmetry of the problem—specifically, they are the relations of the Lie algebra of the relevant symmetry group. An example would be the angular momentum operators, whose commutation relations are those of the Lie algebra of the rotation group SO(3). Typically, the space of states is very far from being irreducible under the pertinent operators, but one can attempt to decompose it into irreducible pieces. In doing so, one needs to know the irreducible representations of the given Lie algebra. In the study of the quantum hydrogen atom, for example, quantum mechanics textbooks give (without calling it that) a classification of the irreducible representations of the Lie algebra .
Structure theory and classification
Lie algebras can be classified to some extent. In particular, this has an application to the classification of Lie groups.
Abelian, nilpotent, and solvable
Analogously to abelian, nilpotent, and solvable groups, defined in terms of the derived subgroups, one can define abelian, nilpotent, and solvable Lie algebras.
A Lie algebra is abelian if the Lie bracket vanishes, i.e. [x,y] = 0, for all x and y in . Abelian Lie algebras correspond to commutative (or abelian) connected Lie groups such as vector spaces or tori, and are all of the form meaning an n-dimensional vector space with the trivial Lie bracket.
A more general class of Lie algebras is defined by the vanishing of all commutators of given length. A Lie algebra is nilpotent if the lower central series
Every finite-dimensional Lie algebra has a unique maximal solvable ideal, called its radical. Under the Lie correspondence, nilpotent (respectively, solvable) connected Lie groups correspond to nilpotent (respectively, solvable) Lie algebras.
A Lie algebra is "simple" if it has no non-trivial ideals and is not abelian. (This implies that a one-dimensional—necessarily abelian—Lie algebra is by definition not simple, even though it has no nontrivial ideals.) A Lie algebra is called semisimple if it is isomorphic to a direct sum of simple algebras. There are several equivalent characterizations of semisimple algebras, such as having no nonzero solvable ideals.
The concept of semisimplicity for Lie algebras is closely related with the complete reducibility (semisimplicity) of their representations. When the ground field F has characteristic zero, any finite-dimensional representation of a semisimple Lie algebra is semisimple (i.e., direct sum of irreducible representations). In general, a Lie algebra is called reductive if the adjoint representation is semisimple. Thus, a semisimple Lie algebra is reductive.
The Levi decomposition expresses an arbitrary Lie algebra as a semidirect sum of its solvable radical and a semisimple Lie algebra, almost in a canonical way. (Such a decomposition exists for a finite-dimensional Lie algebra over a field of characteristic zero.) Furthermore, semisimple Lie algebras over an algebraically closed field have been completely classified through their root systems.
The tangent space of a sphere at a point . If is the identity element, then the tangent space is also a Lie Algebra.
Although Lie algebras are often studied in their own right, historically they arose as a means to study Lie groups.
We now briefly outline the relationship between Lie groups and Lie algebras. Any Lie group gives rise to a canonically determined Lie algebra (concretely, the tangent space at the identity). Conversely, for any finite-dimensional Lie algebra , there exists a corresponding connected Lie group with Lie algebra . This is Lie's third theorem; see the Baker–Campbell–Hausdorff formula. This Lie group is not determined uniquely; however, any two Lie groups with the same Lie algebra are locally isomorphic, and in particular, have the same universal cover. For instance, the special orthogonal groupSO(3) and the special unitary groupSU(2) give rise to the same Lie algebra, which is isomorphic to with the cross-product, but SU(2) is a simply-connected twofold cover of SO(3).
If we consider simply connected Lie groups, however, we have a one-to-one correspondence: For each (finite-dimensional real) Lie algebra , there is a unique simply connected Lie group with Lie algebra .
The correspondence between Lie algebras and Lie groups is used in several ways, including in the classification of Lie groups and the related matter of the representation theory of Lie groups. Every representation of a Lie algebra lifts uniquely to a representation of the corresponding connected, simply connected Lie group, and conversely every representation of any Lie group induces a representation of the group's Lie algebra; the representations are in one-to-one correspondence. Therefore, knowing the representations of a Lie algebra settles the question of representations of the group.
As for classification, it can be shown that any connected Lie group with a given Lie algebra is isomorphic to the universal cover mod a discrete central subgroup. So classifying Lie groups becomes simply a matter of counting the discrete subgroups of the center, once the classification of Lie algebras is known (solved by Cartan et al. in the semisimple case).
If the Lie algebra is infinite-dimensional, the issue is more subtle. In many instances, the exponential map is not even locally a homeomorphism (for example, in Diff(S1), one may find diffeomorphisms arbitrarily close to the identity that are not in the image of exp). Furthermore, some infinite-dimensional Lie algebras are not the Lie algebra of any group.
Given a semisimple finite-dimensional complex Lie algebra , a split form of it is a real form that splits; i.e., it has a Cartan subalgebra which acts via an adjoint representation with real eigenvalues. A split form exists and is unique (up to isomorphisms). A compact form is a real form that is the Lie algebra of a compact Lie group. A compact form exists and is also unique.
Lie algebra with additional structures
A Lie algebra can be equipped with some additional structures that are assumed to be compatible with the bracket. For example, a graded Lie algebra is a Lie algebra with a graded vector space structure. If it also comes with differential (so that the underlying graded vector space is a chain complex), then it is called a differential graded Lie algebra.
Lie rings need not be Lie groups under addition. Any Lie algebra is an example of a Lie ring. Any associative ring can be made into a Lie ring by defining a bracket operator . Conversely to any Lie algebra there is a corresponding ring, called the universal enveloping algebra.
Lie rings are used in the study of finite p-groups through the Lazard correspondence. The lower central factors of a p-group are finite abelian p-groups, so modules over Z/pZ. The direct sum of the lower central factors is given the structure of a Lie ring by defining the bracket to be the commutator of two coset representatives. The Lie ring structure is enriched with another module homomorphism, the pth power map, making the associated Lie ring a so-called restricted Lie ring.
Lie rings are also useful in the definition of a p-adic analytic groups and their endomorphisms by studying Lie algebras over rings of integers such as the p-adic integers. The definition of finite groups of Lie type due to Chevalley involves restricting from a Lie algebra over the complex numbers to a Lie algebra over the integers, and then reducing modulo p to get a Lie algebra over a finite field.
Any Lie algebra over a general ring instead of a field is an example of a Lie ring. Lie rings are notLie groups under addition, despite the name.
Any associative ring can be made into a Lie ring by defining a bracket operator
For an example of a Lie ring arising from the study of groups, let be a group with the commutator operation, and let be a central series in — that is the commutator subgroup is contained in for any . Then
is a Lie ring with addition supplied by the group operation (which is abelian in each homogeneous part), and the bracket operation given by
extended linearly. The centrality of the series ensures that the commutator gives the bracket operation the appropriate Lie theoretic properties.
Boza, Luis; Fedriani, Eugenio M.; Núñez, Juan (2001-06-01). "A new method for classifying complex filiform Lie algebras". Applied Mathematics and Computation. 121 (2–3): 169–175. doi:10.1016/s0096-3003(99)00270-2. ISSN0096-3003.