Abstract
So far we did not worry about how the classical symmetries of a theory are carried over to the quantum theory. We have implicitly assumed that classical symmetries are preserved in the process of quantization.
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Notes
- 1.
In any even number of dimensions \(\gamma_{5}\) is defined to satisfy the conditions \((\gamma_{5})^{2}={\bf 1}\) and \(\{\gamma_{5},\gamma^{\mu}\}=0.\)
- 2.
In fact there is a tension between the conservation of the vector an axial vector currents. The calculation of the diagram shown in Eq. (9.31) can be carried out imposing the conservation of the axial vector current , which results in an anomaly for the vector current. Since this would be disastrous for the consistency of the theory, we choose the other alternative.
- 3.
In the real world this makes sense only for the up and down, and perhaps the strange quarks.
- 4.
The normalization of the generators \(T^{I}\) of the global SU(\(N_{f}\)) is given by \({\rm Tr }(T^{I} T^{J})={\frac{1}{2}}\delta^{IJ}.\)
- 5.
An early computation of the triangle diagram for the electromagnetic decay of the pion was made by Steinberger in [11].
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Álvarez-Gaumé, L., Vázquez-Mozo, M.Á. (2012). Anomalies. In: An Invitation to Quantum Field Theory. Lecture Notes in Physics, vol 839. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-23728-7_9
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