Integration question in Peskin and Schroeder

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SUMMARY

The discussion centers on proving the last step of equation (2.51) in "An Introduction to Quantum Field Theory" by Peskin and Schroeder, specifically the expression for the propagator D(x-y). The participants highlight the use of the method of stationary phase to approach the problem, despite initial confusion regarding the oscillatory nature of the function involved. References to relevant threads provide additional context and clarification, particularly regarding the relationship to Bessel functions.

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ianhoolihan
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Hi all, I'm stuck with proving the last step of (2.51) in Peskin and Schroeder:
$$\begin{align} D(x-y) &= \frac{1}{4\pi^2}\int^\infty_m dE \sqrt{E^2 - m^2}e^{-iEt}\\
& \approx_{t \to \infty}\ \ e^{-imt}\end{align}$$

I've read on another post that the solution is to use the method of stationary phase, but I do not see how this applies, as E is not a rapidly oscillating function...?

Thoughts appreciated,

Ianhoolihan
 
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