The commutator of two elements, g and h, of a groupG, is the element
[g, h] = g−1h−1gh
and is equal to the group's identity if and only if g and h commute (that is, if and only if gh = hg). The set of all commutators of a group is not in general closed under the group operation, but the subgroup of Ggenerated by all commutators is closed and is called the derived group or the commutator subgroup of G. Commutators are used to define nilpotent and solvable groups and the largest abelianquotient group.
The definition of the commutator above is used throughout this article, but many other group theorists define the commutator as
Commutator identities are an important tool in group theory. The expression ax denotes the conjugate of a by x, defined as x−1ax.
Identity (5) is also known as the Hall–Witt identity, after Philip Hall and Ernst Witt. It is a group-theoretic analogue of the Jacobi identity for the ring-theoretic commutator (see next section).
N.B., the above definition of the conjugate of a by x is used by some group theorists. Many other group theorists define the conjugate of a by x as xax−1. This is often written . Similar identities hold for these conventions.
Many identities are used that are true modulo certain subgroups. These can be particularly useful in the study of solvable groups and nilpotent groups. For instance, in any group, second powers behave well:
It is zero if and only if a and b commute. In linear algebra, if two endomorphisms of a space are represented by commuting matrices in terms of one basis, then they are so represented in terms of every basis. By using the commutator as a Lie bracket, every associative algebra can be turned into a Lie algebra.
The anticommutator of two elements a and b of a ring or an associative algebra is defined by
Sometimes is used to denote anticommutator, while is then used for commutator. The anticommutator is used less often, but can be used to define Clifford algebras and Jordan algebras, and in the derivation of the Dirac equation in particle physics.
If A is a fixed element of a ring R, identity (1) can be interpreted as a Leibniz rule for the map given by . In other words, the map adA defines a derivation on the ring R. Identities (2), (3) represent Leibniz rules for more than two factors, and are valid for any derivation. Identities (4)–(6) can also be interpreted as Leibniz rules. Identities (7), (8) express Z-bilinearity.
Some of the above identities can be extended to the anticommutator using the above ± subscript notation.
(For the last expression, see Adjoint derivation below.) This formula underlies the Baker–Campbell–Hausdorff expansion of log(exp(A) exp(B)).
A similar expansion expresses the group commutator of expressions (analogous to elements of a Lie group) in terms of a series of nested commutators (Lie brackets),
The general Leibniz rule, expanding repeated derivatives of a product, can be written abstractly using the adjoint representation:
Replacing x by the differentiation operator , and y by the multiplication operator , we get , and applying both sides to a function g, the identity becomes the usual Leibniz rule for the nth derivative .