MS Renormalization: Questions & Answers

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Discussion Overview

The discussion revolves around the MS renormalization scheme in quantum field theory, specifically addressing the implications of this scheme on the mass in the Lagrangian, the creation and annihilation operators, and the residue of the propagator. Participants explore theoretical aspects and interpretations related to these concepts.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions why the creation and annihilation operators are divided by the square root of the residue of the propagator at the physical mass within the MS renormalization scheme.
  • Another participant explains that if the residue of the pole in the propagator is Z, a factor of Z^(-1/2) is needed for each field in the LSZ formula for scattering amplitude.
  • A third participant references a specific text where it is stated that the renormalized field has unit amplitude to create a one-particle state, raising further questions about the role of the residue in this context.
  • A later reply indicates that the participant reconciled the interpretations of MS and P&S after reviewing the suggested pages, suggesting a personal resolution rather than a consensus in the discussion.

Areas of Agreement / Disagreement

Participants express differing interpretations of the MS renormalization scheme and its implications, with no clear consensus reached on the specific roles of the residue and the renormalized fields.

Contextual Notes

Limitations include potential misunderstandings of the LSZ formula and the specific definitions of terms like residue and renormalized fields, which may vary across different texts.

RedX
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I have a question about the MS renormalization scheme. When you choose this scheme, all sorts of strange things start happening. The mass in your Lagrangian can no longer be the physical mass. The 4-momentum of a physical particle squares to the physical mass, not the free-field mass. But what I don't get is why the creation and annihilation operators get divided by the square root of the residue of the propagator at the physical mass. How does this happen?
 
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I'm not sure I know what you're asking. Very generally, if the residue of the pole in the propagator is Z, then you need a factor of Z^(-1/2) multiplying each field in the LSZ formula for the scattering amplitude. See e.g. P&S eq.(7.42) (where they have Z^(1/2) times the scattering ampliude instead of Z^(-1/2) times the field).
 
I was looking at page 173 of MS's book where he talks about the MS scheme (Mark Srednecki). He writes that " Z^{\frac{-1}{2}}\phi(x) now has unit amplitude to create a one-particle state ".

The creation and annihilation operators are usually the Fourier coefficients of the free-field solutions, solved in terms of the field. But from the derivation of the LSZ forumula, you should really insert the renormalized field into the expression for the creation and annihilation operators, and not the bare fields. But although that might explain factors of Z_{\phi}, how does the residue R come into play?

I'll see if I can find a preview of P&S online from google books - my library doesn't have it.
 
Okay, thanks, I figured it out from those pages of PS you suggested. I like MS's interpretation better, but I only understood what MS was saying after I read the pages of PS you gave. I was able to reconcile MS's and PS's interpretation.
 

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