Solve Peskin's QFT Eqn 2.54 with Hints

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SUMMARY

The discussion focuses on solving Peskin's Quantum Field Theory (QFT) Equation 2.54, which involves transforming a three-dimensional integral into a four-dimensional integral. The key steps include recognizing the role of Dirac delta functions and performing contour integration on the denominator \( p^2 - m^2 \). The solution requires breaking down the denominator to identify poles at \( p^0 = \pm E_p \) and applying the appropriate integration techniques. Participants emphasize the importance of understanding the transition from the three-dimensional to four-dimensional representation in QFT.

PREREQUISITES
  • Quantum Field Theory fundamentals
  • Understanding of Dirac delta functions
  • Contour integration techniques
  • Familiarity with Peskin and Schroeder's QFT textbook
NEXT STEPS
  • Study the derivation of Dirac delta functions in QFT contexts
  • Learn about contour integration in complex analysis
  • Review the transition from three-dimensional to four-dimensional integrals in QFT
  • Examine the implications of poles in integrals for physical interpretations
USEFUL FOR

This discussion is beneficial for graduate students in physics, particularly those studying Quantum Field Theory, as well as researchers seeking to deepen their understanding of integral transformations in QFT.

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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