Is this a mistake in Weinberg's book?

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Discussion Overview

The discussion revolves around a perceived inconsistency in Weinberg's textbook regarding the treatment of variables in a specific equation, particularly the notation used for momentum in relation to the delta function. Participants explore whether this is a mistake or an assumption of prior knowledge expected from readers.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant questions why Weinberg uses ##p' = p## on the right-hand side of an equation but retains ##p'## on the left-hand side, suggesting a possible mistake.
  • Another participant explains that the property ##f(p,p')\delta(p-p')=f(p,p)\delta(p-p')## holds for well-behaved functions, implying that the notation may be justified.
  • Some participants express frustration that Weinberg assumes readers have prior knowledge of delta functions and distributions, indicating a disconnect between the text's expectations and the readers' backgrounds.
  • Others defend Weinberg's approach, stating that the text is aimed at a graduate-level audience and that familiarity with delta functions is a prerequisite for understanding the material.
  • A participant suggests that Weinberg's text is advanced and may not be suitable as a first introduction to quantum field theory (QFT), recommending alternative texts for foundational understanding.

Areas of Agreement / Disagreement

Participants express mixed views on whether Weinberg's treatment is appropriate. Some believe it is reasonable for a graduate-level text, while others feel it is unfair to expect such background knowledge from all readers. The discussion remains unresolved regarding the specific notation in question.

Contextual Notes

Some participants note that the discussion involves assumptions about the reader's background knowledge in quantum field theory and the properties of distributions, which may not be universally held.

kent davidge
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The image is below. My question is, why he considers ##p' = p## on the RHS of ##(2.5.14)## but not on the LHS, i.e., the sub index on the left ##\Psi## remains ##p'##. Is it a mistake? And he continues on the derivation (not shown here) even considering ##|N(p)|^2## instead of ##N(p')^*N(p)## so it doesn't seem like a typo.

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Because ##f(p,p')\delta(p-p')=f(p,p)\delta(p-p')## for any "well behaved" function ##f(p,p')##.
 
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Sounds a little tough that Weinberg supposes we knew that before reading the text.

That's not what I would expect from a serious author
 
kent davidge said:
Sounds a little tough that Weinberg supposes we knew that before reading the text.

But this is what a delta function does.

kent davidge said:
That's not what I would expect from a serious author

Sorry, but I think that this is both untrue and unfair. This is something that I would expect from a serious author of a graduate-level textbook.
 
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kent davidge said:
That's not what I would expect from a serious author

As @George Jones points out, Weinberg's text is a graduate level text. That corresponds to an "A" level thread here at PF. The basic properties of delta functions are indeed part of the background someone would be expected to have for an "A" level discussion here. You labeled this thread as "I", indicating undergraduate level, so it's understandable that you might not have that background; but that just means you are not really the intended audience of Weinberg's text. (Not that that's a problem; taking on a text at a higher level can be a good learning experience. But you should expect to come up against instances like this where the text assumes background knowledge that you don't have, because the text is aimed at a more advanced audience.)
 
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kent davidge said:
Sounds a little tough that Weinberg supposes we knew that before reading the text.

That's not what I would expect from a serious author
Ehm, well, if you start with relativistic QFT you should indeed know fundamental facts about distributions. In physics you almost always only need Dirac's ##\delta## distribution, which is treated on the relevant level in any good textbook on theoretical classical electrodynamics, a subject taught in the 3rd-semester theory-course lecture.

That said, Weinberg is a very advanced textbook, treating many details of QFT in the most general sense (e.g., particles for arbitrary spin). That's why it's unlikely that you understand the subject using it as your first book on QFT. For that purpose, I recommend

M. D. Schwartz, Quantum Field Theory and the Standard Model, Cambridge University Press

Then you can appreciate Weinberg to learn some more subtle details, particularly from a very "practical" point of view, "why QFT is the way it is" (answer: Poincare symmetries+causality). To learn other more subtle details you should also consider the excellent book

A. Duncan, The Conceptual Framework of Quantum Field Theory, Oxford University Press

which has of course a lot of overlap with Weinberg but also treats subjects not found in Weinberg, like "How to stop worrying about Haag's theorem" and some other puzzles of this kind, you always encounter when involved with QFT, which is an addictive subject anyway :-)).
 
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Thank you all for your opinions/replies/advice.
 

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