Learning QFT from Peskin and Schroeder

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Discussion Overview

The discussion revolves around the derivation of the electromagnetic field and its coupling to the Dirac field in quantum field theory (QFT), particularly in relation to gauge invariance as presented in Ryder's work. Participants explore whether similar principles apply to the Dirac field as they do to the complex Klein-Gordon field.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant notes that Ryder shows the electromagnetic field arises from demanding invariance under gauge transformations in the context of the complex Klein-Gordon field and questions if this applies to the Dirac field.
  • Another participant asserts that local gauge invariance for the Dirac field requires a similar transformation, suggesting that the electromagnetic field can also be derived for the Dirac field.
  • A participant claims that this relationship indicates that classical electromagnetism is necessary for local gauge invariance in quantum mechanics and implies that all elementary particles must possess some form of charge.
  • Several participants express admiration for the result, emphasizing its significance and suggesting it deserves more recognition within the field of theoretical physics.
  • References to additional literature, such as Franklin's "Classical Electromagnetism" and Barut's work, are made to support the discussion.

Areas of Agreement / Disagreement

Participants generally express agreement on the significance of the result regarding gauge invariance and its implications for the Dirac field, but the discussion does not reach a consensus on the broader recognition of this result within the physics community.

Contextual Notes

Some participants reference specific sections of texts and suggest that the argument may be presented differently in various sources, indicating a potential for differing interpretations or approaches to the topic.

Son Goku
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I'm still pretty new to QFT, so forgive me if I have made a ridiculous mistake.

I've been learning QFT from Peskin and Schroeder mostly but decided to read Ryder recently and I have just come across an amazing result (in my opinion) in Chapter 3.

Ryder basically shows that the electromagnetic field and its coupling to the complex Klein Gordon Field "arises naturally by demanding invariance of the action under gauge transformation of the second kind in the internal space of the complex Klein Gordon field".

My question is, does this also hold for the Dirac Field?

By making similar demands on the Dirac Field can one derive the electromagnetic field and its coupling to the Dirac Field?

(Hopefully I haven't written this in a difficult to understand manner)
 
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Son Goku said:
I'm still pretty new to QFT, so forgive me if I have made a ridiculous mistake.

I've been learning QFT from Peskin and Schroeder mostly but decided to read Ryder recently and I have just come across an amazing result (in my opinion) in Chapter 3.

Ryder basically shows that the electromagnetic field and its coupling to the complex Klein Gordon Field "arises naturally by demanding invariance of the action under gauge transformation of the second kind in the internal space of the complex Klein Gordon field".

My question is, does this also hold for the Dirac Field?

By making similar demands on the Dirac Field can one derive the electromagnetic field and its coupling to the Dirac Field?

(Hopefully I haven't written this in a difficult to understand manner)
Yes for Dirac. In order to have Local Gauge Invariance for the Dirac field,
\partial_\mu\rightarrow\partial_\mu-eA^\mu is required, just as for the KG field.
 
In fact, that shows that classical EM theory is required by LGI in QM,
and that all truly elementary particles (other than the gauge particles themselves) must have some kind of charge. It also shows why charge is intrinsicly dimensionless.
 
Thanks. That is an unbelievably powerful result.
I still can't get over the idea that electromagnetism can be "derived".

Thanks again.
 
Meir Achuz said:
In fact, that shows that classical EM theory is required by LGI in QM,
and that all truly elementary particles (other than the gauge particles themselves) must have some kind of charge. It also shows why charge is intrinsicly dimensionless.


I agree with Son Goku; this is a marvelous result! Why isn't it better known, broadcast to the hills as one of the triumphs of field theory? You could write a whole popular book around this one topic (with intro; I'm thinking of something which motivates an unrigorous notion of partial derivative, etc.).
 
selfAdjoint said:
I agree with Son Goku; this is a marvelous result! Why isn't it better known, broadcast to the hills as one of the triumphs of field theory? You could write a whole popular book around this one topic (with intro; I'm thinking of something which motivates an unrigorous notion of partial derivative, etc.).
This is done in the last chapter of "Classical Electromagnetism" by Franklin.
 
Meir Achuz said:
This is done in the last chapter of "Classical Electromagnetism" by Franklin.

Thanks! I just ordered a used copy of it online, because I want very much to study the argument used.
 
I believe the same argument is made in A. O. Barut, Electrodynamics and the Classical Theory of Fields and Particles, section IV.3.
 

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