The commutator of operators and
is
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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 vector fields and let
be a torsion-free connection.
Then their Lie bracket satisfies
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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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where
is the identity matrix. Then
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(13)
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