Solving Schwartz QFT Eqn 5.26 to Get Eqn 5.27

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SUMMARY

The discussion focuses on the transition from Equation 5.26 to Equation 5.27 in Schwartz's Quantum Field Theory (QFT) textbook. Equation 5.26 is expressed as dΠ_{LIPS}=(2π)^{4} δ^{4}(Σp) (d^{3}p_{3}/(2π)^{3})(1/2E_{3})(d^{3}p_{4}/(2π)^{3})(1/2E_{4}), while Equation 5.27 simplifies this to dΠ_{LIPS}=(1/16π^{2}) dΩ ∫ dp_{f} (p_{f}^{2}/E_{3})(1/E_{4}) δ(E_{3}+E_{4}-E_{CM}). The key steps involve integrating over the delta function and switching to spherical coordinates in momentum space. The discussion also highlights the importance of Lorentz invariance and the specific frame adopted in Equation 5.27.

PREREQUISITES
  • Understanding of Quantum Field Theory (QFT) concepts
  • Familiarity with delta functions in physics
  • Knowledge of momentum space and spherical coordinates
  • Experience with Lorentz invariance in particle physics
NEXT STEPS
  • Study the derivation of delta functions in Quantum Field Theory
  • Learn about momentum space transformations and their applications
  • Explore the implications of Lorentz invariance in particle interactions
  • Review advanced QFT textbooks, such as Aitchison and Hey, for deeper insights
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Students and researchers in theoretical physics, particularly those focusing on Quantum Field Theory and particle physics, will benefit from this discussion.

merrypark3
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Hello.
From Schwartz QFT BOOK,
How could Eqn 5.26 can be Eqn 5.27?

d \Pi_{LIPS}=(2 \pi) ^{4} \delta^{4}(\Sigma p) \frac{d^{3} p_{3}}{(2 \pi) ^{3}} \frac{1}{2 E_{3}} \frac{d^{3} p_{4}}{(2 \pi)^{3}} \frac{1}{2 E_{4}} Eqn(5.26)


d \Pi_{LIPS}=\frac{1}{16 \pi ^{2}} dΩ ∫ d p_{f} \frac{{p_{f}}^2}{E_{3}} \frac{1}{E_{4}} \delta ( E_{3} + E_{4} - E_{CM}) Eqn(5.27)
 
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Just integrate over the ##\delta##-function and then switch to spherical coordinates in momentum space. Keep in mind ##\delta^4 (\Sigma p) = \delta^4 (p^{\mu}_1 + p^{\mu}_2 - p^{\mu}_3 - p^{\mu}_4)## so separate the ##\delta##-function into products over the 3-vectors and the energies.
 
Integrate over? In (5.26), there is no integration?
 
It's implicit.
 
Yeah, there really shouldn't be an integral sign in 5.27 if there isn't one in 5.26. Also, p_3 has changed its name to p_f. Also, while 5.27 is Lorentz invariant, he's adopted a specific frame (the CM frame) in 5.27.
 
OK. as \vec{p_{3}}=-\vec{p_{4}} , we can insert integration (over \vec{p_{4}} ) in Eqn(5.26) without altering the original. got it.
 
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thanks. I would ask some more questions about Shwartz QFT textbook. I hope to solve all the exercises of this book within 2 years, though had solved only up to ch.4
 
merrypark3 said:
I hope to solve all the exercises of this book within 2 years, though had solved only up to ch.4

Cool, well good luck! I'm working through the book as well actually. I'm on ch.7 problems. So it looks like we have the same goals :)
 
Good. Good luck! This book is quite well written.
 
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merrypark3 said:
This book is quite well written.

Haha yes, it is the first QFT book I've personally come across that actually feels like a true physics book. It almost feels like cheating having this book in possession when my class's assigned text is (unfortunately) Peskin and Schroeder since the former provides all the intuition that the latter completely lacks, at least in Part I (I haven't even looked Parts II and beyond).

EDIT: actually Aitchison and Hey is a really awesome physics book as well, George Jones told me about it.
 
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