Clarification on Lie Derivatives

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SUMMARY

The Lie derivative of a vector field X along another vector field Y is defined as $$\mathcal{L}_Y X = \lim_{t\to 0} \frac{X_{\phi(t)} - \phi_{t*}X}{t}$$, where ##\phi_t## is the flow generated by Y. The expressions $$\mathcal{L}_Y X = [Y,X]$$ and $$\mathcal{L}_Y X = \nabla_Y X - \nabla_X Y$$ are equivalent under specific conditions. Specifically, (1) and (2) hold true when the connection ##\nabla## is torsion-free, and the equivalence of (*) with (1) or (2) depends on the vanishing of torsion, defined as T(X,Y) = ##\nabla_X Y - \nabla_Y X - [X,Y]##.

PREREQUISITES
  • Understanding of vector fields and flows in differential geometry.
  • Familiarity with the concept of Lie derivatives.
  • Knowledge of connections and torsion in differential geometry.
  • Proficiency in calculus, particularly limits and derivatives.
NEXT STEPS
  • Study the properties of Lie derivatives in various geometrical contexts.
  • Learn about torsion-free connections and their implications in differential geometry.
  • Explore the relationship between Lie derivatives and curvature.
  • Investigate the applications of Lie derivatives in physics, particularly in general relativity.
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Mathematicians, physicists, and students of differential geometry seeking to deepen their understanding of Lie derivatives and their applications in various fields.

center o bass
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The standard definition of the lie derivative of X along Y is just

$$(*) \mathcal{L}_YX = \lim_{t\to 0} \frac{X_{\phi(t)} - \phi_{t*}X}{t}$$

where ##\phi_t## is the flow generated by Y. I.e. the limit of the difference between a pushforward of X along Y and X evaluated at a point ##\phi(t)## on the flow of Y. Other than this definition I have seen the expressions

$$(1) \mathcal{L}_Y X = [Y,X]$$

and

$$(2) \mathcal{L}_YX = \nabla_Y X - \nabla_X Y$$

for the Lie Derivative, but I have not seen it stated clearly when (1) and (2) holds. Surely (1) and (2) is equivalent when the connection ##\nabla## is torsion free. However is it generally true that (*) is equivalent with (1) or (2)? What conditions on ##\nabla## must be satisfied in order to identify (*) with (1) (or (2))?
 
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center o bass said:
The standard definition of the lie derivative of X along Y is just

$$(*) \mathcal{L}_YX = \lim_{t\to 0} \frac{X_{\phi(t)} - \phi_{t*}X}{t}$$

where ##\phi_t## is the flow generated by Y. I.e. the limit of the difference between a pushforward of X along Y and X evaluated at a point ##\phi(t)## on the flow of Y. Other than this definition I have seen the expressions

$$(1) \mathcal{L}_Y X = [Y,X]$$

and

$$(2) \mathcal{L}_YX = \nabla_Y X - \nabla_X Y$$

for the Lie Derivative, but I have not seen it stated clearly when (1) and (2) holds. Surely (1) and (2) is equivalent when the connection ##\nabla## is torsion free. However is it generally true that (*) is equivalent with (1) or (2)? What conditions on ##\nabla## must be satisfied in order to identify (*) with (1) (or (2))?

(1) and (*) are equivalent, you should be able to show this.

(2) is equivalent to (1) if and only if the torsion vanishes. In fact, the torsion is defined as the difference between (2) and (1):

T(X,Y) \equiv \nabla_X Y - \nabla_Y X - [X,Y]
 

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