The commutator of two elements, g and h, of a group G, is the element
- [g, h] = g−1h−1gh.
It is equal to the group's identity if and only if g and h commute (i.e., if and only if gh = hg). The subgroup of G generated by all commutators is called the derived group or the commutator subgroup of G. Note that one must consider the subgroup generated by the set of commutators because in general the set of commutators is not closed under the group operation. Commutators are used to define nilpotent and solvable groups.
The above definition of the commutator is used by some group theorists, as well as throughout this article. However, many other group theorists define the commutator as
Identities (group theory)
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.
A wide range of 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
If the derived subgroup is central, then
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 with respect to one basis, then they are so represented with respect to 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 the brackets [ ]+ are also used. The anticommutator is used less often than the commutator, but can be used for example to define Clifford algebras, Jordan algebras and is utilised to derive the Dirac equation in particle physics.
In physics, this is an important overarching principle in quantum mechanics. The commutator of two operators acting on a Hilbert space is a central concept in quantum mechanics, since it quantifies how well the two observables described by these operators can be measured simultaneously. The uncertainty principle is ultimately a theorem about such commutators, by virtue of the Robertson–Schrödinger relation. In phase space, equivalent commutators of function star-products are called Moyal brackets, and are completely isomorphic to the Hilbert-space commutator structures mentioned.
Identities (ring theory)
The commutator has the following properties:
- , where is the anticommutator defined above.
If A is a fixed element of a ring ℜ, the second additional relation can also be interpreted as a Leibniz rule for the map given by B ↦ [A,B]. In other words, the map DA defines a derivation on the ring ℜ.
The following identity ("Hadamard Lemma") involving nested commutators, underlying the Campbell–Baker–Hausdorff expansion of log (exp A exp B), is also useful:
Use of the same expansion expresses the above Lie group commutator in terms of a series of nested Lie bracket (algebra) commutators,
These identities differ slightly for the anticommutator (defined above)
Graded rings and algebras
When dealing with graded algebras, the commutator is usually replaced by the graded commutator, defined in homogeneous components as
Especially if one deals with multiple commutators, another notation turns out to be useful involving the adjoint representation:
- Derivation (abstract algebra)
- Pincherle derivative
- Poisson bracket
- Moyal bracket
- Canonical commutation relation
- Ternary commutator
- Fraleigh, John B. (1976), A First Course In Abstract Algebra (2nd ed.), Reading: Addison-Wesley, ISBN 0-201-01984-1
- Griffiths, David J. (2004), Introduction to Quantum Mechanics (2nd ed.), Prentice Hall, ISBN 0-13-805326-X
- Herstein, I. N. (1964), Topics In Algebra, Waltham: Blaisdell Publishing Company, ISBN 978-1114541016
- Liboff, Richard L. (2003), Introductory Quantum Mechanics (4th ed.), Addison-Wesley, ISBN 0-8053-8714-5
- McKay, Susan (2000), Finite p-groups, Queen Mary Maths Notes 18, University of London, ISBN 978-0-902480-17-9, MR 1802994