Solve Peskin's QFT Eqn 2.54 with Hints

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Homework Help Overview

The discussion revolves around understanding equation 2.54 from Peskin's introductory quantum field theory text. The original poster expresses confusion regarding the derivation of this equation and suspects the involvement of Dirac delta functions.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss rewriting a three-dimensional integral as a four-dimensional integral and suggest performing contour integration to understand the derivation. There are questions about the specific equation being referenced and the steps leading to it.

Discussion Status

Some participants have offered guidance on how to approach the problem, including suggestions to break down the denominator and perform integrals. There is acknowledgment of the need for clarity on the specific equation in question, indicating a productive direction in the discussion.

Contextual Notes

The original poster notes a lack of understanding of the equation and expresses uncertainty about their current approach. There is also a mention of needing to clarify the equation being discussed, which may affect the direction of the conversation.

ananya J
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QFT Peskin p.30 eqn 2.54

Homework Statement



i am perplexed with eqn 2.54 peskins introductory qft. just can't make out how to arrive at it from the previous step. i think that there are dirac delta funtions involved but simply can't make it out. can somebody help? provide some hint? thanks in advance for ur time

3. The Attempt at a Solution
\int\ \frac{d^3p} {(2\pi)^3}\ \{ \frac {1}{2E_p}\ e^{-ip.(x-y)}\left|_{p^0 = E_p}\ +\ \frac {1}{-2E_p}\ e^{-ip.(x-y)}\left|_{p^0 = -E_p}\ \}= \int\ \frac{d^3p} {(2\pi)^3}\ \int\ \frac{dp^0} {2p^0}\ e^{-ip.(x-y)}\ \{ \delta (p_0-E_p) +\delta (p_0+E_p)\ \} = \int\ \frac{d^3p} {(2\pi)^3}\ \int\ dp^0\ e^{-ip.(x-y)}\ \delta(p^2-m^2)

dont know if iam on the right track.pls correct me if am wrong.
 
Last edited:
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It would be good, if you would write down the equation you want to prove, since I don't have the mentioned book...
 
What P&S are doing in Eqn. 2.54 is re-writing a three-dimensional integral as a four-dimensional integral:
\int\frac{d^3p}{(2\pi)^3}\frac{1}{2E_p}[\exp(-ip\cdot(x - y)) - \exp(ip\cdot (x - y))] = \int\frac{d^3p}{(2\pi)^3}\int\frac{dp^0}{2\pi i}\ \frac{-1}{p^2 - m^2}\exp(-ip\cdot(x - y)),
where x^0 > y^0.

What I would do to understand this is start from the latter form and perform the p^0 integral. Break up the denominator into
p^2 - m^2 = (p^0)^2 - \textbf p^2 - m^2,
which has poles at
p^0 = \pm \sqrt{\textbf p^2 + m^2} = \pm E_p.
Contour integration should produce the first expression in the original post [which P&S give as an intermediate step] without too much trouble.
 
i jumped into conclusions before reading the text further. sorry. anyways thanks so much for ur time & help.:smile:
 
Last edited:

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