Anomaly of representations in SU(N)

In summary, an anomaly of representations in SU(N) is a violation of symmetry at the quantum level in a quantum field theory. It can arise when the path integral measure used to calculate quantum amplitudes is not invariant under certain transformations, and can have various consequences such as making the theory not well-defined or causing conflicts with experimental data. It is possible to cancel an anomaly of representations in SU(N) by including additional fields or symmetries in the theory, and scientists study these anomalies through theoretical calculations and experimental observations.
  • #1
nickthequick
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Homework Statement



The problem is the following: Compute the ratio of the anomaly of the N to that of the N(N-1)/2 representations in SU(n)

Homework Equations



Georgi claims that you can find the anomaly, A(R) of the [1] representation of SU(n) by calculating the anomaly of SU(3) (subgroup of SU(N)) under which n transforms like a 3 and n-3 singlets.

The Attempt at a Solution



The anomaly of the fundamental rep is going to be 1 here in SU(3). I'm not exactly sure how to find the anomaly of the (n-3) singlets. Also, if I do attain A([1]) for SU(N), I'm not sure how to extend this to the other N and N(N-1)/2 reps.

Any insights would be appreciated.

Cheers
 
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  • #2

Thank you for your post. This is an interesting problem that requires some knowledge of group theory and representation theory. To compute the ratio of the anomaly of the N to that of the N(N-1)/2 representations in SU(n), we can use the following formula:

A(R) = Tr(F^2) - Tr(R^2)

where A(R) is the anomaly of the representation R, Tr(F^2) is the trace of the generator of the group in the representation, and Tr(R^2) is the trace of the quadratic Casimir operator in the representation.

To find the anomaly of the fundamental representation [1] in SU(n), we can use the formula A([1]) = Tr(F^2) - Tr([1]^2) = n - 1, where n is the dimension of the group. This is because the fundamental representation has n-1 generators and the quadratic Casimir operator in this representation is n-1.

To find the anomaly of the (n-3) singlets, we can use the fact that the anomaly of a direct product representation is the sum of the anomalies of the individual representations. Therefore, the anomaly of the (n-3) singlets will be (n-3)(-1) = 3-n.

Now, to extend this to the other representations, we can use the formula A(R) = Tr(F^2) - Tr(R^2). For the N representation, we have A(N) = Tr(F^2) - Tr(N^2) = n - Tr(N^2). Similarly, for the N(N-1)/2 representation, we have A(N(N-1)/2) = Tr(F^2) - Tr(N(N-1)/2)^2 = n - Tr(N(N-1)/2)^2.

To find the ratio of the anomalies, we can use the fact that the trace of a direct product representation is the product of the traces of the individual representations. Therefore, the ratio of the anomalies will be:

A(N)/A(N(N-1)/2) = (n - Tr(N^2))/(n - Tr(N(N-1)/2)^2)

I hope this helps. Good luck with your calculations!
 

1. What is an anomaly of representations in SU(N)?

An anomaly of representations in SU(N) refers to a situation where the symmetry of a quantum field theory is not preserved at the quantum level. This means that the theory is not invariant under certain transformations, even though it may appear to be at the classical level.

2. How does an anomaly of representations in SU(N) arise?

An anomaly of representations in SU(N) can arise when the path integral measure used to calculate quantum amplitudes is not invariant under certain transformations. This can happen when the theory has chiral fermions or when the gauge group is non-Abelian.

3. What are the consequences of an anomaly of representations in SU(N)?

The consequences of an anomaly of representations in SU(N) vary depending on the particular theory and symmetry involved. In some cases, it may mean that the theory is not well-defined and cannot be consistently quantized. In other cases, it may lead to unexpected physical effects or conflicts with experimental data.

4. Can an anomaly of representations in SU(N) be canceled?

In certain cases, it is possible to cancel an anomaly of representations in SU(N) by including additional fields or symmetries in the theory. This cancellation is known as an 'anomaly cancellation' and is an active area of research in theoretical physics.

5. How do scientists study anomalies of representations in SU(N)?

Scientists study anomalies of representations in SU(N) through theoretical calculations and experimental observations. They use mathematical tools such as group theory and path integrals to analyze the symmetry structure of a theory and look for any anomalies. They also use data from particle accelerators and other experiments to test the predictions of these theories and see if any anomalies are present.

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