Definition of the Lie derivative

In summary: In particular, if ##Y = \frac{\partial}{\partial x_i}##, then ##\phi_{t*}Y = \frac{\partial}{\partial \phi_t(x)_i}##.
  • #1
spaghetti3451
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Consider the Lie derivative of the vector field ##\bf{Y}## with respect to the vector field ##\bf{X}## on manifold ##M^{n}(x)## defined as

##\displaystyle{[\mathcal{L}_{\bf{X}}Y]_{x}:=\lim_{t\rightarrow 0} \frac{[{\bf{Y}}_{\phi_{t}x}-\phi_{t*}{\bf{Y}}_{x}]}{t}}##

Now, I understand that ##{\bf{Y}}_{\phi_{t}x}## is the tangent vector of the vector field ##\bf{Y}## at the point ##\phi_{t}x##, where the point ##\phi_{t}x## is obtained by starting at point ##x## at time ##0## and traversing along the orbit of ##x## to time ##t##.

But I don't understand how to interpret ##\phi_{t*}{\bf{Y}}_{x}##. Given the map ##\phi_{t}## which maps points ##x## in ##M^{n}## to points ##\phi_{t}(x)## in ##M^{n}## along the orbit of ##x## parameterised by time ##t##, we can define the differential ##\phi_{t*}## that maps the tangent vector of the vector field ##Y## at ##x## to some tangent vector at the point ##\phi_{t}x##. Now, there is only one tangent vector of the vector field ##\bf{Y}## at the point ##\phi_{t}x##, and this tangent vector is the vector ##{\bf{Y}}_{\phi_{t}x}##. This seems to suggest that ##{\bf{Y}}_{\phi_{t}x}## and ##\phi_{t*}{\bf{Y}}_{x}##.

What am I missing?
 
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  • #2
Not sure what you mean by the phrase "tangent vector of the vector field". But anyway:

##Y_{\phi_t x}## is the vector that lives at ##\phi_t x##, whereas ##\phi_{t*} Y_x## is the vector that lives at ##x##, pushed forward by the flow ##\phi## to the point ##\phi_t x##.

If you imagine vectors as tiny arrows living on your manifold, then the pushforward ##\phi_{t*}## acts by pushing both the head and the tail of the little arrow along the flow lines. So, the little arrow ##\phi_{t*} Y_x## is completely defined in terms of the little arrow ##Y_x## that lives at ##x##, given the flow ##\phi_t##.

In contrast, the little arrow ##Y_{\phi_t x}## is the one that was already sitting at ##\phi_t x## to begin with, and hasn't been pushed along the flow.
 
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  • #3
Just to put mathematics on what Ben said: ##\phi_t## defines a function from the manifold to itself. Any such function defines a map from the tangent space at ##x## to the tangent space at ##\phi_t(x)##. Taking ##X \in T_x M##, ##\phi_{t*}X## is defined by ##\phi_{t*}X[f] = X[f \circ \phi_t]## (note that ##f(\phi_t(x))## is a function on the manifold as long as ##f## is).
 

FAQ: Definition of the Lie derivative

What is the definition of the Lie derivative?

The Lie derivative is a mathematical operation in differential geometry that describes how a tensor field changes along a vector field.

How is the Lie derivative calculated?

The Lie derivative is calculated as the rate of change of a tensor field along a vector field, measured by the Lie bracket of the vector field and the tensor field.

What is the significance of the Lie derivative in physics?

The Lie derivative is used to describe the evolution of physical quantities in a spacetime, making it an important tool in general relativity and other areas of theoretical physics.

Can the Lie derivative be extended to other mathematical objects?

Yes, the Lie derivative can be extended to act on a variety of mathematical objects, including differential forms, vector fields, and tensors of any valence.

Why is the Lie derivative useful in studying symmetries?

The Lie derivative is closely related to symmetry transformations, and it is useful in studying symmetries because it allows us to describe how a given tensor field changes when the underlying space is transformed by a symmetry operation.

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