Lie Derivatives  

In General > s.a. Derivatives.
* Idea: A notion of directional derivative on an arbitrary differentiable manifold that depends on a vector field va, but not on a choice of connection (it is a concomitant).
* Useful formula: For any p-form (p > 1),

v = v · d + d(v · ) .

* Lie derivatives of the coordinate basis elements:

v(/xi) = –(vj/xi) (/xj) ,   v (dxi) = (vi/xj) dxj .

* Other properties: Acting on forms, it commutes with taking the exterior derivative, d(v ) = v(d).

For Various Types of Fields > s.a. spin coefficients; spin structures.
* Scalar functions: Coincides with other notions of derivative,

v f |x:= limt to 0 t–1 [f(t(x)) – f(x)] = v(f)|x va a f |x .

* Vector fields: Defined using the push-forward under the diffeomorphisms generated by va,

v w|x:= limt to 0 t–1 [t–1'(w(t(x))) – w(x)] = [v,w]x .

* One-forms: Defined using the pull-back under the diffeomorphisms generated by va,

v |x:= limt to 0 t–1 [t*((t(x))) – (x)] .

* Arbitrary tensor fields: Defined implicitly by the product rule v (M N) = v M N + M v N; e.g.,

v Mac:= vm m MacMmc mva + Mam cvm .

* Scalar/tensor densities of weight 1:

v f = va a f + f a va = a (va f) ;   v M = |g|1/2 v M + (div v) M .

* With torsion: Includes additional terms; For example,

v Xa = vm m XaXm m va vm Xn Tmna .

* Spinor fields: Defined only if va is a Killing vector field, otherwise one would have to define some Lie derivative of a pair spinor-metric somehow; It is given by v := va a + (a kb) ab .

Related Concepts
* Lie bracket: The Lie derivative induces a Lie bracket structure on vector fields,

[v, w] = v w .

@ References: Crainic & Fernandes AM(03) [integrability].

References
@ General: Schouten 54 [red threads embedded in gelatin]; Yano 55.
@ For spinor fields: Kosmann AMPA(71); Hurley & Vandyck JPA(94), JPA(94), JPA(95) [and covariant derivative]; Fatibene et al gq/96-in; Ortín CQG(02)ht [all spins]; Godina & Matteucci IJGMP(05)m.DG.
@ Generalized framework: Hurley & Vandyck JMP(01).
> Online resources: see Wikipedia page.


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