Wilson Line Propagator: Understanding Eqtn 5.7 & 5.8

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Discussion Overview

The discussion revolves around the interpretation and implications of equations 5.7 and 5.8 in the context of the Wilson line propagator. Participants explore the behavior of exponential functions at infinity and the convergence of integrals, particularly focusing on the treatment of limits and undefined terms.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions the treatment of the exponential term with an imaginary component at infinity in Eqtn 5.7, suggesting that the textbook implies it is zero despite sine and cosine being undefined at infinity.
  • Another participant proposes introducing a small variable ##\epsilon > 0## to ensure convergence of the integral in Eqtn 5.7, allowing the exponential to vanish as ##\lambda## approaches negative infinity.
  • A subsequent post reiterates the introduction of ##\epsilon## and raises concerns about the undefined nature of terms resulting from this limit, particularly regarding the lower limit of integration.
  • One participant argues that the limit should be taken at the end of calculations, implying that the exponential terms will not affect the results until then.
  • Another participant clarifies that the upper limit of the integral in Eqtn 5.6 is 0, which leads to an exponential term of 1, questioning the earlier claims about the upper limit's contribution.

Areas of Agreement / Disagreement

Participants express differing views on the treatment of exponential functions at infinity and the implications of introducing the variable ##\epsilon##. The discussion remains unresolved regarding the final contributions of the exponential terms in the equations.

Contextual Notes

There are unresolved questions about the handling of limits, the behavior of exponential functions at infinity, and the implications of the introduced variable ##\epsilon##. The discussion highlights the complexity of these mathematical treatments without reaching a consensus.

Elmo
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TL;DR
An undefined term in the wilson line propagator
I asked this from a number of people but no one knew what to do about this exponential with iota infinity in the power,in Eqtn 5.7
The textbook seems to imply that it is zero but cos and sine are undefined at infinity.
Also,all the exponentials seem to vanish from the final result of Eqtn 5.8 whereas the integration of exponential function should still leave behind the function.
Where do all the exponentials go ?
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I think the author intoduces a small variable ##\epsilon > 0## so to write the integral in 5.7 as:

$$\lim_{\epsilon \rightarrow 0^+} \int_{-\infty}^{\lambda_2} d\lambda e^{-i(nk + i \epsilon)\lambda}$$

In this way you will have your original exponential multiplied by ##e^{\epsilon \lambda}##. This will assure the convergence of the function as ##\lambda## goes to ##-\infty## because it will exponentially go to zero.
The result of the integral is to be understood with a ##\lim_{\epsilon \rightarrow 0^+}## in front.
 
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dRic2 said:
I think the author intoduces a small variable ##\epsilon > 0## so to write the integral in 5.7 as:

$$\lim_{\epsilon \rightarrow 0^+} \int_{-\infty}^{\lambda_2} d\lambda e^{-i(nk + i \epsilon)\lambda}$$

In this way you will have your original exponential multiplied by ##e^{\epsilon \lambda}##. This will assure the convergence of the function as ##\lambda## goes to ##-\infty## because it will exponentially go to zero.
The result of the integral is to be understood with a ##\lim_{\epsilon \rightarrow 0^+}## in front.
Seems good though it introduces another undefined term as the lower limit, in the form of
$$e^{-n\epsilon\infty} $$
And as ##\epsilon \rightarrow 0## is being multiplied with infinity ,should that not again be undefined ?
Also,my other question remains that what happens to the exponentials in the upper limit ?
Why don't they show up in the final expression or the list of Feynman rules.
 
Elmo said:
should that not again be undefined
No. You take the ##\lim_{\epsilon->0^+}## at the end of all the calculations. So, first, you do the definite integral (that is first you take the limit as ##\lambda \rightarrow - \infty## which annihilates the exponential).

As for your second question, I don't see it immediately. If I have time I'll check more carefully. Sorry
 
Elmo said:
Also,my other question remains that what happens to the exponentials in the upper limit ?
You are performing the integrals in (5.6) one after the other. The explicit example is for the innermost one (over ##\lambda_1##). Have you verified the claim about the ##\lambda_2## integral? The upper limit in the last integral (the leftmost integral symbol) is 0, giving you ##e^0 = 1##.
 

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