In mathematics, the commutator gives an indication of the extent to which a certain binary operation fails to be commutative. Mathematics is the body of Knowledge and Academic discipline that studies such concepts as Quantity, Structure, Space and In Mathematics, a binary operation is a calculation involving two Operands, in other words an operation whose Arity is two In Mathematics, commutativity is the ability to change the order of something without changing the end result There are different definitions used in group theory and ring theory. Group theory is a mathematical discipline the part of Abstract algebra that studies the Algebraic structures known as groups. In Mathematics, ring theory is the study of rings, Algebraic structures in which addition and multiplication are defined and have similar properties to those
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The commutator of two elements g and h of a group G is the element
It is equal to the group's identity if and only if g and h commute (i. In Mathematics, a group is a set of elements together with an operation that combines any two of its elements to form a third element 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. In Group theory, given a group G under a Binary operation * we say that some Subset H of G is a subgroup of In Mathematics, more specifically in Abstract algebra, the commutator subgroup or derived subgroup of a group is the Subgroup 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. In Group theory, a nilpotent group is a group having a special property that makes it "almost" abelian, through repeated application of the In the history of Mathematics, the origins of Group theory lie in the search for a proof of the general unsolvability of Quintic and higher equations finally
N. B. The above definition of the commutator is used by group theorists. Many other mathematicians define the commutator as
In the sequel the expression ax denotes the conjugated (by x) element x−1a x.
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. The second identity is also known under the name Hall-Witt identity. It is a group-theoretic analogue of the Jacobi identity for the ring-theoretic commutator (see next section). The fourth identity follows from the first and third.
N. B. The above definition of the conjugate of a by x is used by group theorists. Many other mathematicians define the conjugate of a by x as xax−1. This is usually written xa.
The commutator of two elements a and b of a ring or an associative algebra is defined by
It is zero if and only if a and b commute. In Mathematics, a ring is an Algebraic structure which generalizes the algebraic properties of the Integers though the rational, real In Mathematics, an associative algebra is a Vector space (or more generally a module) which also allows the multiplication of vectors in a distributive 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. Linear algebra is the branch of Mathematics concerned with By using the commutator as a Lie bracket, every associative algebra can be turned into a Lie algebra. Lie bracket can refer to Lie algebra Lie bracket of vector fields In Mathematics, a Lie algebra is an algebraic structure whose main use is in studying geometric objects such as Lie groups and differentiable Manifolds Lie The commutator of two operators defined on a Hilbert space is an important concept in quantum mechanics since it measures how well the two observables described by the operators can be measured simultaneously. This article assumes some familiarity with Analytic geometry and the concept of a limit. Quantum mechanics is the study of mechanical systems whose dimensions are close to the Atomic scale such as Molecules Atoms Electrons In Physics, particularly in Quantum physics, a system observable is a property of the system state that can be determined by some sequence of physical The uncertainty principle is ultimately a theorem about these commutators. In Quantum physics, the Heisenberg uncertainty principle states that locating a particle in a small region of space makes the Momentum of the particle uncertain In Mathematics, a theorem is a statement proven on the basis of previously accepted or established statements
The commutator has the following properties:
Lie-algebra relations:
![[A,A] = 0 \,\!](../../../../math/f/1/d/f1dae2493b8868b4af71b12cfcbbf2a2.png)
![[A,B] = - [B,A] \,\!](../../../../math/f/e/a/fea063199da61c9481eb11030e07a42d.png)
![[A,[B,C]] + [B,[C,A]] + [C,[A,B]] = 0 \,\!](../../../../math/1/e/3/1e3f33da2c7e5a55d058ba099493d50b.png)
The second relation is called anticommutativity, while the third is the Jacobi identity. In mathematics anticommutativity refers to the property of an operation being anticommutative, i In Mathematics the Jacobi identity is a property that a binary operation can satisfy which determines how the order of evaluation behaves for the given operation
Additional relations:
![[A,BC] = [A,B]C + B[A,C] \,\!](../../../../math/d/2/0/d203fa5bb12e2872f4f048bc2e61fe42.png)
![[AB,C] = A[B,C] + [A,C]B \,\!](../../../../math/8/e/2/8e21d0d3e0b281bbcc53717af824e1ad.png)
![[A,BC] = [AB,C] + [CA,B] \,\!](../../../../math/a/d/f/adf8b176c47621ad6a73386c83252474.png)
![[ABC,D] = AB[C,D] + A[B,D]C + [A,D]BC \,\!](../../../../math/9/0/4/904f75dfe250a4fa8ff148d674a7f436.png)
![[[[A,B], C], D] + [[[B,C], D], A] + [[[C, D], A], B] + [[[D, A], B], C] = [[A, C], [B, D]] \,\!](../../../../math/9/a/0/9a02636cb5b160ba766a31f6f1cd0633.png)
If A is a fixed element of a ring
, the first additional relation can also be interpreted as a Leibniz rule for the map
given by
. In other words: the map DA defines a derivation on the ring
. In Abstract algebra, a derivation is a function on an algebra which generalizes certain features of the Derivative operator
The following identity involving commutators, a special case of the Baker-Campbell-Hausdorff formula, is also useful:
![e^{A}Be^{-A}=B+[A,B]+\frac{1}{2!}[A,[A,B]]+\frac{1}{3!}[A,[A,[A,B]]]+...](../../../../math/3/2/c/32c59da4c0a12b661a1cfaa719a3cc79.png)
When dealing with graded algebras, the commutator is usually replaced by the graded commutator, defined in homogeneous components as ![\ [\omega,\eta]_{gr} := \omega\eta - (-1)^{\deg \omega \deg \eta} \eta\omega](../../../../math/3/c/8/3c89e3ce16977e52a6154f60deedbb55.png)
Especially if one deals with multiple commutators, another notation turns out to be useful involving the adjoint representation:
![\operatorname{ad} (x)(y) = [x, y] .](../../../../math/7/1/9/719dbc343123eb48f0f7c61d5b48c6ce.png)
Then ad(x) is a derivation and ad is linear, i. In Mathematics, the Baker-Campbell-Hausdorff formula is the solution to Z = \log(e^X e^Y\ for non- commuting X In Mathematics, in particular Abstract algebra, a graded algebra is an Algebra over a field (or Commutative ring) with an extra piece of structure In Mathematics, the adjoint representation (or adjoint action) of a Lie group G is the natural representation of G on its In Abstract algebra, a derivation is a function on an algebra which generalizes certain features of the Derivative operator e. , ad(x + y) = ad(x) + ad(y) and
, and a Lie algebra homomorphism, i. In Mathematics, a Lie algebra is an algebraic structure whose main use is in studying geometric objects such as Lie groups and differentiable Manifolds Lie e, ad([x,y]) = [ad(x),ad(y)], but it is not always an algebra homomorphism, i. e the identity
does not hold in general.
Examples:
![{\rm ad} (x){\rm ad} (x)(y) = [x,[x,y]\,]](../../../../math/2/9/e/29e4c9f866cc624e64da2dcdd73205ad.png)
![{\rm ad} (x){\rm ad} (a+b)(y) = [x,[a+b,y]\,]](../../../../math/0/d/6/0d6201de9b808b26dedb20c5a537153f.png)