Propagator using cauchy integral

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Discussion Overview

The discussion revolves around the derivation of propagator expressions using the Cauchy integral, specifically focusing on the evaluation of integrals involving the step function and the choice of contour paths in complex analysis. Participants explore the implications of different values of tau (τ) on the contour integration process.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions the rationale behind choosing contour paths above or below the real axis when evaluating the integral for different values of tau (τ).
  • Another participant suggests that the choice of contour depends on the sign of tau, indicating that the semicircle contour's contribution is relevant to the evaluation.
  • A later reply clarifies that for τ < 0, the contour integral can be taken above the real axis, as the upper semicircle does not contribute to the integral due to Jordan's lemma, leading to a zero result consistent with the step function.
  • Participants express confusion about the justification for ignoring singularities in certain cases, particularly when τ < 0.
  • There is a mention of evaluating the cases of τ > 0 and τ < 0 separately to demonstrate the behavior of the step function.

Areas of Agreement / Disagreement

Participants express uncertainty and confusion regarding the justification for contour choices in the integral evaluation. There is no consensus on the explanation of why certain paths can be chosen or why singularities can be ignored in specific cases.

Contextual Notes

Participants highlight the dependence on the sign of tau and the implications of Jordan's lemma, but the discussion does not resolve the underlying assumptions or the mathematical steps involved in the contour integration process.

Gary Weiss
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hi
I don't understand this bit about the derivation of propagator expressions.
Bjorken and Drell describe the step function as:
[tex]\theta(\tau)=lim_{\epsilon \to 0}\frac{-1}{2\pi i}\oint_{-\infty}^{\infty}\frac{d\omega e^{-i\omega r}}{\omega + i \epsilon }[/tex]

the singularity is at [tex]-i \omega \epslion[/tex]

I understand that if I evaluate this integral with a path above the real axis
I get zero, and that if I evaluate it below the real axis I get 1.

however I don't understand why it's ok to choose the paths in this way.
What happened at tau<0 that allowed me to integrate only the upper half of
the real/imaginary axis?

thanks!
 
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Gary Weiss said:
hi
I don't understand this bit about the derivation of propagator expressions.
Bjorken and Drell describe the step function as:
[tex]\theta(\tau)=lim_{\epsilon \to 0}\frac{-1}{2\pi i}\oint_{-\infty}^{\infty}\frac{d\omega e^{-i\omega r}}{\omega + i \epsilon }[/tex]

the singularity is at [tex]-i \omega \epslion[/tex]

I understand that if I evaluate this integral with a path above the real axis
I get zero, and that if I evaluate it below the real axis I get 1.

however I don't understand why it's ok to choose the paths in this way.
What happened at tau<0 that allowed me to integrate only the upper half of
the real/imaginary axis?

thanks!

Consider the case [tex]\tau >0[/tex] and [tex]\tau <0[/tex] separately.
The choice the upper semicircle contour or the lower semicircle contour depends on the sign of [tex]\tau[/tex], i.e. if the semicircle part of the contour contributed, that's not the original contour integral you want to calculate.

Calculate these two cases separately, you will see that's exactly step function.
 
sorry I don't get it...
why is it that when tau < 0 I can choose the contour above the real axis and ignore the singularity.
 
Gary Weiss said:
sorry I don't get it...
why is it that when tau < 0 I can choose the contour above the real axis and ignore the singularity.


When \tau <0, you contour integral is equivalent to the closed contour integral which goes above the real axis.(because the upper semicircle doesn't contribute to the integral, this is ensured by Jordan's lemma)

Since there is no pole inside the contour, the integral is zero, consistent with step function.

You can consider the case when \tau>0.
It would give you one.
 

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