How to work with a non-Abelian gauge field

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Homework Help Overview

The discussion revolves around non-Abelian gauge fields in quantum field theory (QFT). The original poster expresses confusion regarding the transformations of the gauge field A(x) and the role of the partial derivative in these transformations. They question whether the partial derivative should act on the transformation U or be treated as a constant, as well as the treatment of A(x) and F(x) as operators.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the nature of the transformation U in the context of SU(2) models, questioning whether U is constant or varies. There is discussion about the implications of treating U as a local gauge transformation and the effects on the partial derivative.

Discussion Status

Some participants have provided references to literature, such as Chris Quigg's book, to guide understanding of the transformations. There is an ongoing exploration of the assumptions regarding the behavior of U and its derivatives, but no consensus has been reached on the specific interpretations.

Contextual Notes

The original poster's background is unclear, which may affect the depth of the discussion. The conversation is constrained by the complexity of the topic and the need for further clarification on specific terms and concepts in non-Abelian gauge theory.

jtceleron
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Homework Statement


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Homework Equations


I am learning QFT, and I am confused of such transformations. For example, first, in these equations, especially the one that defines the transformation of A(x), whether should the partial derivative acts on U(or U-1), or just take U as a constant? Second, the partial derivative acts only on U-1 or all the things after it?
Another question is should we consider A(x) and F(x) as an operator, so that when calculating, it is convenient to put a function after it.

The Attempt at a Solution

 

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I am not sure about your background but if you want to show it then you can take a simple say SU(2) model,and note that the U's are not constant .In most representation it can be modeled as,U=exp(ζata).you can look up here for this and most noteworthy is chriss quigg book on every kind of interactions.
https://docs.google.com/viewer?a=v&q=cache:rIlRjFXgsUgJ:www.staff.science.uu.nl/~wit00103/ftip/Ch12.pdf+non+abelian+gauge+field+theory&hl=en&gl=in&pid=bl&srcid=ADGEEShqJlXAn76qqji-voYWnDTnSwkJelRaIib5JXx5oLZGhl30sk1OqYHIo2GTAQBaBfT6RQyAyl3itZF7VAYITk8vDdTHbp2BjVoK1NwdzydbX0ZkAEyvea3rkpV9U90W8FYs1XuP&sig=AHIEtbRTdHObuHKb1PeRx73K-wOszayn0Q
 
andrien said:
I am not sure about your background but if you want to show it then you can take a simple say SU(2) model,and note that the U's are not constant .In most representation it can be modeled as,U=exp(ζata).you can look up here for this and most noteworthy is chriss quigg book on every kind of interactions.
https://docs.google.com/viewer?a=v&q=cache:rIlRjFXgsUgJ:www.staff.science.uu.nl/~wit00103/ftip/Ch12.pdf+non+abelian+gauge+field+theory&hl=en&gl=in&pid=bl&srcid=ADGEEShqJlXAn76qqji-voYWnDTnSwkJelRaIib5JXx5oLZGhl30sk1OqYHIo2GTAQBaBfT6RQyAyl3itZF7VAYITk8vDdTHbp2BjVoK1NwdzydbX0ZkAEyvea3rkpV9U90W8FYs1XuP&sig=AHIEtbRTdHObuHKb1PeRx73K-wOszayn0Q
You mean that, for example, in the last equation of transformation for A(x), the partial derivative should act on U-1, rather than taking U-1 as a constant?
 
jtceleron said:
You mean that, for example, in the last equation of transformation for A(x), the partial derivative should act on U-1, rather than taking U-1 as a constant?

Yes,of course because U used here as a local gauge transformation.the transformation of gradient takes the form
μψ=U∂μψ+(∂μU)ψ
For the derivation which you are looking for,I will refer you to chris quigg book on'gauge theory of strong,weak,electromagnetic' page 55-60.I am not going to derive it here because as always I am out of time.
 

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