Lie derivative (for vector fields)


Let M be a smooth manifoldMathworldPlanetmath, and X,Y∈𝒯⁢(M) smooth vector fields on M. Let Θ:𝒰→M be the flow of X, where 𝒰⊆ℝ×M is an open neighborhood of {0}×M. We make use of the following notation:

𝒰p={t∈ℝ|(t,p)∈𝒰},∀p∈M,
𝒰t={p∈M|(t,p)∈𝒰},∀t∈ℝ,

and we introduce the auxiliary maps θt:𝒰t→M and θp:𝒰p→M defined as

Θ⁢(t,p)=θt⁢(p)=θp⁢(t),∀(t,p)∈𝒰.

The Lie derivativeMathworldPlanetmathPlanetmath of Y along X is the vector field ℒX⁢Y∈𝒯⁢(M) defined by

(ℒX⁢Y)p=dd⁢t⁢(d⁢(θ-t)θt⁢(p)⁢(Yθt⁢(p)))|t=0=limt→0⁡d⁢(θ-t)θt⁢(p)⁢(Yθt⁢(p))-Ypt,∀p∈M,

where d⁢(θ-t)θt⁢(p)∈Hom⁢(Tθt⁢(p)⁢M,Tp⁢M) if the push-forward of θ-t, i.e.

d⁢(θ-t)θt⁢(p)⁢(v)⁢(f)=v⁢(f∘θ-t),∀v∈Tθ-t⁢(p)⁢M,f∈C∞⁢(p).

The following result is not immediate at all.

Theorem 1

ℒX⁢Y=[X,Y], where [X,Y]=X⁢Y-Y⁢X is the Lie bracket of X and Y.

Title Lie derivative (for vector fields)
Canonical name LieDerivativeforVectorFields
Date of creation 2013-03-22 14:09:59
Last modified on 2013-03-22 14:09:59
Owner matte (1858)
Last modified by matte (1858)
Numerical id 9
Author matte (1858)
Entry type Definition
Classification msc 53-00
Defines Lie derivative