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Given a smooth manifold X, the Lie bracket of vector fields u and v can be defined in several ways.
Since derivations of smooth functions are vector fields, we can identify u and v with the corresponding derivations C∞(X)→C∞(X).
Taking the commutator uv−vu of these derivations produces another derivation, which is denoted by [u,v], and which can be identified with a vector field on X.
Alternatively, we can set
[u,v]=ℒuv=ℒvu,where ℒ denotes the Lie derivative of a vector field.
The real vector space of vector fields on X equipped with the Lie bracket forms a Lie algebra.
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