Coordinate representation of a diffeomorphism

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Discussion Overview

The discussion revolves around the mathematical concept of diffeomorphisms generated by vector fields, focusing on the representation of these transformations in coordinate systems. Participants explore the integration of vector fields along parametrized paths on manifolds and the implications of differentiating these expressions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant proposes that the coordinates for the point ##Y_X(\lambda)## can be computed through integration of the vector field, suggesting the expression: ##Y^\alpha_X(\lambda) = X^\alpha + \int V^\alpha|_{Y_X(\lambda)} d\lambda##.
  • Another participant questions the validity of this approach, arguing that it requires solving a system of differential equations rather than simple integration, using an example from ##\mathbb R^2## to illustrate the complexity of the relationships involved.
  • There is a discussion about whether the expression for the vector field's dependence should involve the covariant derivative ##\nabla_\mu V^\alpha## or if a partial derivative suffices, with some participants expressing uncertainty regarding the implications of connections in this context.
  • Concerns are raised about the interchangeability of integration and differentiation in the context of the parametrized path, with a suggestion to apply the chain rule when differentiating the vector field along the path.
  • One participant acknowledges the ability to express the equations in integral form but emphasizes that they remain unsolved equations, highlighting the dependence on initial conditions.

Areas of Agreement / Disagreement

Participants express differing views on the nature of the integration process and the necessity of solving differential equations, indicating a lack of consensus on the approach to representing diffeomorphisms in coordinate systems.

Contextual Notes

Limitations include the potential misunderstanding of the relationship between integration and differentiation in this context, as well as the dependence on initial conditions that complicates the integration process.

stevendaryl
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I'm trying to understand diffeomorphisms, and I thought I basically understood them, but when I tried to work out a problem I created for myself, I realized I didn't know how to answer it.

So let's consider a diffeomorphism generated by a vector field ##V##. If ##X## is a point on our manifold, then we can define a parametrized path ##Y_X(\lambda)## via:

##Y_X(0) = X##

##\frac{d}{d\lambda} Y_X(\lambda) = V|_{Y_X(\lambda)}##

So far, ##X## and ##Y## are points on the manifold, not coordinates, but now I'd like to switch to a coordinate system. I'll just use ##X^\alpha## and ##Y^\alpha## to mean the coordinates of points ##X## and ##Y##, and use ##V^\alpha## to mean the components of ##V## in the coordinate basis for our coordinate system.

The first uncertainty on my part is whether the following is true:

If we want to know the coordinates for the point ##Y_X(\lambda)##, I think it's just a matter of integration:

##Y^\alpha_X(\lambda) = Y^\alpha_X(0) + \int V^\alpha|_{Y_X(\lambda)} d\lambda##
## = X^\alpha + \int V^\alpha|_{Y_X(\lambda)} d\lambda##

Assuming that is correct, what I want to compute next is the dependence of ##Y^\alpha_X(\lambda)## on ##X##. At this point, my first inclination would be:

##\frac{\partial Y^\alpha_X(\lambda)}{\partial X^\beta} = \frac{\partial X^\alpha}{\partial X^\beta}+ \int \frac{\partial V^\alpha}{\partial Y^\mu}|_{Y_X(\lambda)} \frac{\partial Y^\mu_X(\lambda)}{\partial X^\beta} d\lambda##

My uncertainty is with the expression ##\frac{\partial V^\alpha}{\partial Y^\mu}##. Should that be ##\nabla_\mu V^\alpha## rather than the partial derivative? My feeling is that it shouldn't be, since the concept of diffeomorphism is independent of whether there is a connection, or not.
 
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I would have written the integration as ##Y_X(\lambda) = Y_X(0) + \int_0^\lambda V(Y_X(\mu)) \,d\mu## locally around ##\lambda = 0##.

So the first question is, whether ##\left(\int_0^\lambda V(Y_X(\mu)) \,d\mu \right)^\alpha = \int_0^\lambda V^\alpha(Y_X(\mu)) \,d\mu \,## and next whether integration and (partial) differentiation can be switched. If both is true, then we get ##\dfrac{\partial V^\alpha}{\partial X^\beta} = \dfrac{\partial V^\alpha (Y_X(\mu))}{\partial X^\beta}## and we have to apply the chain rule on ##V^\alpha \circ Y_X##.
 
stevendaryl said:
The first uncertainty on my part is whether the following is true:

If we want to know the coordinates for the point ##Y_X(\lambda)##, I think it's just a matter of integration:

##Y^\alpha_X(\lambda) = Y^\alpha_X(0) + \int V^\alpha|_{Y_X(\lambda)} d\lambda##
## = X^\alpha + \int V^\alpha|_{Y_X(\lambda)} d\lambda##

If I understand correctly your question and notations, I think this is not true. It will not be just integration, you need to solve a system of differential equations. Take any example. Say ##\mathbb R^2## with the usual coordinates ##(x,y)##, let the vector field be ##V=x^2\frac{\partial}{\partial x}+y\frac{\partial}{\partial y}##. Then the parametrized path you are looking for satisfies
##\frac{dx}{d\lambda}=x^2##
##\frac{dy}{d\lambda}=y##
Solving the equations is not just a matter of integration. Well in a way it is because I chose them simple to solve, but in general the right sides will depend on all coordinate function, they will not be decoupled as in this example. The dependence on the initial point will come from the initial conditions for the equations ##x(0)=x_0## and ##y(0)=y_0##.
 
martinbn said:
If I understand correctly your question and notations, I think this is not true. It will not be just integration, you need to solve a system of differential equations. Take any example. Say ##\mathbb R^2## with the usual coordinates ##(x,y)##, let the vector field be ##V=x^2\frac{\partial}{\partial x}+y\frac{\partial}{\partial y}##. Then the parametrized path you are looking for satisfies
##\frac{dx}{d\lambda}=x^2##
##\frac{dy}{d\lambda}=y##
Solving the equations is not just a matter of integration. Well in a way it is because I chose them simple to solve, but in general the right sides will depend on all coordinate function, they will not be decoupled as in this example. The dependence on the initial point will come from the initial conditions for the equations ##x(0)=x_0## and ##y(0)=y_0##.

Very good point. However, I would say it is true that ##x(\lambda) = x(0) + \int_0^{\lambda} V^x(x(s), y(s)) ds##, but unhelpful. My question is not about how to solve it, but about the meaning.
 
I see, I have misunderstood you question. Yes, you are right, that you can write the equations in that form (as integral equations), but they are still equations, as the unknown appears on both sides. They are not solved.
 

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