Confusion about the Z factor(Renormalization factor)

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SUMMARY

The discussion centers on the Z factor, or field-strength renormalization factor, as described in Peskin's textbook, specifically in chapter 7 on Radiative Corrections. It is established that the Z factor is irrelevant for calculations at the leading order of perturbation theory, where it equals 1, but becomes significant in higher-order corrections. The irrelevance at leading order is attributed to the electron self-energy being zero, which leads to a Z value of 1. The need for renormalization arises from the non-analytic behavior of Z in relation to the coupling constant, resulting in divergences when Taylor expanded.

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  • Understanding of perturbation theory in quantum field theory
  • Familiarity with renormalization concepts
  • Knowledge of self-energy calculations in quantum electrodynamics
  • Basic grasp of Taylor series expansions and their implications in physics
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This discussion is beneficial for theoretical physicists, particularly those specializing in quantum field theory, as well as students seeking to deepen their understanding of renormalization and perturbation theory.

phylz
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In Peskin's textbook chapter 7 Radiative Corrections: Some formal developments (page 229), he said the Z factors are irrelevant for calculations at the leading order of perturbation theory, but are important in the calculation or higher-order corrections.

My question is how can the Z factor be irrelevant for calculations at the leading order of perturbation theory. Thanks.
 
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phylz said:
In Peskin's textbook chapter 7 Radiative Corrections: Some formal developments (page 229), he said the Z factors are irrelevant for calculations at the leading order of perturbation theory, but are important in the calculation or higher-order corrections.

My question is how can the Z factor be irrelevant for calculations at the leading order of perturbation theory. Thanks.

Z is the field-strength renormalization factor
 
At the lowest order in perturbation theory it is just ##1##.
 
DarMM said:
At the lowest order in perturbation theory it is just ##1##.
@DarMM thank you. Now I got it, for electron, $Z_2^(-1)=1-\frac{d\Sigma}{d\slashed{p}}|_{\slashed{p}=m}$, at the leading-order contribution, electron self-energy is 0, so Z=1.
 
Yes exactly. Note that the singularities in ##Z## and hence the need to renormalise it arise from the fact that ##Z## is not analytic in the coupling constant, so Taylor expanding it causes divergences.
 

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