Lie bracket
The Lie bracket is an anticommutative, bilinear, first order differential operator on vector fields. It may be defined either in terms of local coordinates or in a global, coordinate-free fashion. Though both defintions are prevalent, it is perhaps easier to formulate the Lie Bracket without the use of coordinates at all, as a commutator:
Definition (Global, coordinate-free) Suppose and are vector fields on a smooth manifold . Regarding these vector fields as operators on functions, the Lie bracket is their commutator:
Definition (Local coordinates) Suppose and are vector fields on a smooth -dimensional manifold , suppose are local coordinates around some point , and suppose that in these local coordinates
Then the Lie bracket of the above vector fields is the locally defined vector field
(The Einstein summation convention employed in the above equations — repeated indices are to be summed from the range 1 to .)
Properties
Suppose are smooth vector fields on a smooth manifold .
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where is the Lie derivative.
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is anti-symmetric and bi-linear.
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Vector fields on with the Lie bracket is a Lie algebra. That is to say, the Lie bracket satisfies the Jacobi identity:
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The Lie bracket is covariant with respect to changes of coordinates.
Title | Lie bracket |
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Canonical name | LieBracket |
Date of creation | 2013-03-22 14:10:02 |
Last modified on | 2013-03-22 14:10:02 |
Owner | rspuzio (6075) |
Last modified by | rspuzio (6075) |
Numerical id | 10 |
Author | rspuzio (6075) |
Entry type | Definition |
Classification | msc 53-00 |
Related topic | HamiltonianAlgebroids |