Smart Algebra of Exp. on Pg 191 of Peskin & Schroeder

Click For Summary
SUMMARY

The discussion focuses on the algebraic manipulation of the vertex correction function as presented on page 191 of Peskin & Schroeder. The expression involves the left-hand side (LHS) and right-hand side (RHS) formulations, with specific terms like ##m^2## and ##(1-2z-z^2)m^2##. Key relationships include the definitions of the spinors ##\bar{u}(p')## and ##u(p)##, and the application of the Dirac equation to simplify terms. The user successfully resolved the algebraic challenge and plans to share their working for reference.

PREREQUISITES
  • Understanding of quantum field theory concepts, particularly vertex corrections.
  • Familiarity with the Dirac equation and its implications for spinors.
  • Knowledge of Peskin & Schroeder's "An Introduction to Quantum Field Theory" as a reference text.
  • Basic algebraic manipulation skills in the context of quantum mechanics.
NEXT STEPS
  • Study the derivation of vertex corrections in quantum electrodynamics (QED).
  • Learn about the on-shell condition and its applications in quantum field theory.
  • Explore the implications of the Dirac equation on spinor algebra.
  • Review advanced techniques in algebraic manipulation within quantum field theory contexts.
USEFUL FOR

Physicists, graduate students in quantum field theory, and researchers working on particle interactions and vertex corrections will benefit from this discussion.

mdb71
Messages
5
Reaction score
3
Hi all, I have a problem working out the algebra of the following expression in Peskin & Schroeder in a smart way to give the result. It is on page 191, regarding the numerator of the vertex correction function.
We want to get from the LHS to the RHS of the following expression
$$\bar{u}(p')[-\frac{1}{2}l^2\gamma^\mu + (z\not{p}-y\not{q})\gamma^{\mu}(z\not{p}+(1-y)\not{q}) + m^2\gamma^{\mu}-2m((1-2y)q^{\mu}+2zp^{\mu})]u(p)$$ $$ = \bar{u}(p')[\gamma^{\mu}(-\frac{1}{2}l^2+(1-x)(1-y)q^2+(1-2z-z^2)m^2)+(p'^{\mu}+p^{\mu})mz(1-z)+q^{\mu}m(z-2)(x-y)]u(p)$$
using
$$ q \equiv p'-p, \not{p}u(p) = mu(p), \bar{u}(p')\not{p'} = m\bar{u}(p'), \bar{u}(p')\not{q}u(p) = 0,\\
x+y+z = 1$$

Thanks a lot in advance!
 
Physics news on Phys.org
In the LHS you have ##m^2##, while in the RHS you have ##(1-2z-z^2)m^2##. What is the relation between ##\bar{u}(p')## (LHS) and ##u(p')## (RHS)?
 
mathman said:
In the LHS you have ##m^2##, while in the RHS you have ##(1-2z-z^2)m^2##. What is the relation between ##\bar{u}(p')## (LHS) and ##u(p')## (RHS)?
The argument of u is p, not p'. What do you mean what is their relation? They are spinors coming from the vertices which the propagators are attached. However, this is irrelevant; what is important here is the on shell identity - coming from the Dirac equation - by which we may simplify terms...
 
Just solved; I'll post the scan of the working in the next few days just for reference as it is quite an annoying passage. Other than that, feel free to post your answers, it is an opportunities to see some smart tricks at play
 

Similar threads

  • · Replies 0 ·
Replies
0
Views
2K
  • · Replies 13 ·
Replies
13
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 6 ·
Replies
6
Views
4K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 8 ·
Replies
8
Views
4K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 2 ·
Replies
2
Views
4K