Let , 
, ... be operators. Then the
 commutator of 
 and 
 is defined as
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(1)
 
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Let , 
, ... be constants, then identities include
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(2)
 
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(3)
 
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(4)
 
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(5)
 
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(6)
 
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(7)
 
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(8)
 
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Let  and 
 be tensors. Then
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(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
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(10)
 
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(11)
 
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(12)
 
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then
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(13)
 
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