Understanding the Relationship Between Lie Algebras and Lie Groups

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Lie algebras are defined as non-associative structures, which contrasts with the associative nature of groups. The relationship between Lie algebras and Lie groups is established through the tangent space at the identity of the group, representing left invariant vector fields. The Lie bracket, which is the commutator of vector fields, differs from the group multiplication operation. This distinction clarifies how a Lie algebra can describe a Lie group locally despite its non-associative property. Understanding this relationship is crucial in the study of differential geometry and theoretical physics.
Lapidus
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How come that a Lie algebra is defined as being non-associative and at same time it describes a Lie group locally? I wonder because groups are, again by definition, asscioative.

thanks
 
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Let

<br /> a \otimes b \equiv [a, b] = a b - b a<br />

Then:

<br /> a \otimes (b \otimes c) = [a,[b,c]] = [a, b c] - [a, c b] = a b c - b c a - a c b + c b a<br />

But:

<br /> (a \otimes b) \otimes c = [[a, b], c] = [a b, c] - [b a, c] = a b c - c a b - b a c + c b a<br />

These two expressions are not the same. Thus, the operation \otimes is not associative. But, the Lie algebra is precisely defined through such an operation.
 
Lapidus said:
a Lie algebra is defined as being non-associative and at same time it describes a Lie group locally?
The way it "describes a Lie group locally" is somewhat involved. In any case, the product operation of the Lie group and the bracket operation of the corresponding Lie algebra are by no means the same. Specifically, for a Lie group G, the corresponding Lie algebra is the tangent space of G at the identity, which 'is' the space of left invariant vector fields. The Lie bracket is the usual commutator of two vector fields. This is an entirely different operation than the group multiplication of G.

For more information, see wikipedia.
 
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