Path ordered integral over simplices?

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Discussion Overview

The discussion revolves around the derivation of the parallel propagator as presented in Carroll's notes, specifically focusing on the integral in equation 3.40. Participants explore the nature of the integral over simplices versus n-cubes and the conditions for path ordering in the context of parallel propagation in differential geometry.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions why the integral is defined over a simplices instead of an n-cube, suggesting that the limits of integration imply a different structure.
  • Another participant proposes that the orientation of the individual A maps could affect the integral's outcome, hinting at a potential issue with the integral's correctness if not handled properly.
  • A participant speculates that the condition \(\eta_n \geq \eta_{n-1} \geq \ldots \geq \eta_1\) relates to the iteration process in solving for the parallel propagator, indicating a connection to the structure of the integrals involved.
  • Further clarification is provided regarding the nature of the A maps, suggesting they represent infinitesimal parallel propagation along a curve.
  • Another participant notes that the requirement for \(\eta_n \geq \eta_{n-1} \geq \ldots \geq \eta_1\) leads to the use of simplices, as it constrains the integration limits in a way that aligns with the properties of simplices.

Areas of Agreement / Disagreement

Participants express differing views on the nature of the integral and the implications of the ordering condition, indicating that multiple competing interpretations exist without a clear consensus.

Contextual Notes

The discussion includes assumptions about the behavior of the A maps and the implications of their orientation, which are not fully resolved. The connection between the integral's structure and the properties of simplices versus n-cubes remains open to interpretation.

ianhoolihan
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Hi all,

I am trying to follow the derivation by Carroll of the parallel propagator in http://preposterousuniverse.com/grnotes/grnotes-three.pdf notes, beginning page 66 or so.

My question is with the integral in equation 3.40.

1) why is it that this is an integral over a simplice, and not an n-cube (which the limits of integration seem to suggest)?

2) why is it that \eta_n \geq \eta_{n-1}\geq \ldots \geq \eta_1 so that path ordering must take place? (See between equations 3.40 and 3.41 for discussion.)

Cheers,

Ianhoolihan
 
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Hey ianhoolihan.

I can't answer your question specifically, but one thing that you may want to think about is the actual final map that your products of your individual A maps would do to your integral for each simplex.

My guess is that the orientation would be screwed up completely for one and this would affect the integral in a bad way and not give the right result.

Just out of curiosity, what does your linear map A represent?
 
chiro said:
I can't answer your question specifically, but one thing that you may want to think about is the actual final map that your products of your individual A maps would do to your integral for each simplex.

My guess is that the orientation would be screwed up completely for one and this would affect the integral in a bad way and not give the right result.

Just out of curiosity, what does your linear map A represent?

Hmmm, the A maps are (I'm guessing here) an infinitesimal "parallel propagation" in the direction tangent to the curve \gamma. As for the product of the maps, I'm not sure.

I wonder if the reason for \eta_n \geq \eta_{n-1}\geq \ldots \geq \eta_1 is to do with the iteration process...actually, I think that might be it. For those not looking at the pdf, the solution for the parallel propagator is

{P^\mu}_\rho (\lambda,\lambda_0) = {\delta^\mu}_\rho + \int^\lambda_{\lambda_0} {A^\mu}_\sigma(\eta) {P^\sigma}_\rho(\eta,\lambda_0) d\eta

So solving by iteration,

{P^\mu}_\rho (\lambda,\lambda_0) = {\delta^\mu}_\rho +\int^\lambda_{\lambda_0} {A^\mu}_\rho(\eta)d \eta+ \int^\lambda_{\lambda_0} \int^\eta_{\lambda_0} {A^\mu}_\sigma(\eta){A^\sigma}_\rho(\eta')d\eta d\eta' + \ldots

The point being that, in the first equation it is {P^\sigma}_\rho(\eta,\lambda_0), so the next substitution must only range from \eta to \lambda_0, if you understand the abuse of language.

Yup, I think that works.

Now, for the simplices...oh, maybe it follows from \eta_n \geq \eta_{n-1}\geq \ldots \geq \eta_1 quite obviously. For example, in the second term, the integral is over both \eta,\eta' such that \eta' \leq \eta. Hence, simplices.

Thank you.
 
I don't think I did much to warrant a thank-you, but I'm glad you got it in the end.
 

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