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Let , , ... be operators. Then the commutator of and is defined as
![[A^~,B^~]=A^~B^~-B^~A^~.](/images/equations/Commutator/NumberedEquation1.gif) |
(1)
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Let , , ... be constants.
Identities include
Let and be tensors. Then
![[A,B]=del _AB-del _BA.](/images/equations/Commutator/NumberedEquation2.gif) |
(9)
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There is a related notion of commutator in the theory of groups. The commutator of two group elements and is ,
and two elements and are said to commute when their commutator is the identity element. When the group
is a Lie group, the Lie bracket in its Lie
algebra is an infinitesimal version of the group commutator. For instance, let
and be square matrices,
and let and be paths
in the Lie group of nonsingular matrices which satisfy
then
![partial/(partials)partial/(partialt)alpha(s)beta(t)alpha^(-1)(s)beta^(-1)(t)|_((s=0,t=0))=2[A,B].](/images/equations/Commutator/NumberedEquation3.gif) |
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Portions of this entry contributed by Todd
Rowland
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