What are some common questions about Peskin's QFT book?

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Discussion Overview

The discussion revolves around questions raised by participants regarding concepts in chapter 2 of Peskin's Quantum Field Theory (QFT) book. The topics include the microcausality condition, contour integration, and Lorentz transformations related to spacelike separated points. The scope includes theoretical understanding and clarification of concepts presented in the text.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants inquire whether the vanishment of the commutator of fields [\phi(x),\phi(y)]=0 is a postulate and if it relates to microcausality.
  • One participant asserts that this condition is indeed the microcausality condition.
  • Questions are raised about the derivation of microcausality, with some expressing doubt about its derivability from the text.
  • Participants discuss how to prove that for spacelike separated points x and y, there exists a continuous Lorentz transformation that takes x-y to -(x-y), referencing a spacelike vector V.
  • There is a suggestion that transforming V into -V may require not only a rotation but also a boost due to the flipping of the temporal coordinate.
  • One participant mentions that while the microcausality condition can be derived for specific representations like the Fock representation, there is no general way to derive it.

Areas of Agreement / Disagreement

Participants generally agree that the vanishment of the commutator is related to microcausality, but there is uncertainty regarding whether it can be derived as a postulate. The discussion about the Lorentz transformation remains unresolved, with differing views on the necessity of a boost in addition to a rotation.

Contextual Notes

Some participants note that the book does not clearly assert the status of microcausality as a postulate, leading to differing interpretations. The discussion also highlights the complexity of transformations involving spacelike and timelike vectors, indicating that assumptions about the nature of these vectors may affect the conclusions drawn.

ismaili
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Dear all,

While I was reading chap2 of Peskin, I got some questions.
(1) The vanishment of the commutator of fields [\phi(x),\phi(y)]=0 means that the measurements at x and y do not interfere at all. Is this a postulate? Is this the so-called micro-causality?

(2) How Peskin deform the contour of fig.2.3 ? Why the two contour integrals are the same?

(3) How to prove if x,y are space-like separated, there is a continuous Lorentz transformation take x-y to -(x-y)? i.e. I don't understand fig.2.4.

Thanks for anyone.
 
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ismaili said:
While I was reading chap2 of Peskin, I got some questions.
(1) The vanishment of the commutator of fields [\phi(x),\phi(y)]=0 means that the measurements at x and y do not interfere at all. Is this a postulate? Is this the so-called micro-causality?
Yes, this is the microcausality condition.

ismaili said:
(3) How to prove if x,y are space-like separated, there is a continuous Lorentz transformation take x-y to -(x-y)? i.e. I don't understand fig.2.4.
If they are spacelike separated you can define a spacelike vector V that connects them. Then, you can easily show that there exists a Lorentz transformation that transforms V into -V. This will be a rotation of 180 degrees. If you try the same procedure for two points within the light-cone, connected by a timelike vector, you will see that the transformation is not possible.
 
hellfire said:
Yes, this is the microcausality condition.
Thanks. I guessed this is a "postulate", however, the book didn't give a clear assertion that this is a postulate. So I doubt that this can be derived. Now I think it is a postulate of QFT.
hellfire said:
If they are spacelike separated you can define a spacelike vector V that connects them. Then, you can easily show that there exists a Lorentz transformation that transforms V into -V. This will be a rotation of 180 degrees. If you try the same procedure for two points within the light-cone, connected by a timelike vector, you will see that the transformation is not possible.

Thanks, I got it. But it seems that the argument have to be slightly modified. If V is a spacelike vector, we need not only the rotation to transform V into -V. Because the temporal coordinate is flipped too, so I guess we need a boost also.

Thanks for the discussion!
 
ismaili said:
Thanks. I guessed this is a "postulate", however, the book didn't give a clear assertion that this is a postulate. So I doubt that this can be derived. Now I think it is a postulate of QFT.
I started a thread a time ago with a similar question. You may want to use the search function to find it. It seems it is actually a postulate: it can be derived for specific representations such as the Fock representation that, however, restricts itself to positive mass solutions. There is no general way to derive it.

ismaili said:
Thanks, I got it. But it seems that the argument have to be slightly modified. If V is a spacelike vector, we need not only the rotation to transform V into -V. Because the temporal coordinate is flipped too, so I guess we need a boost also.
Yes, but I think that a boost will not do the work to completely transform V into -V if it is timelike.
 

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