Abstract
This chapter applies the material of the previous chapters to some particular topics, specifically the Wigner–Eckart theorem, selection rules, and gamma matrices and Dirac bilinears. We begin by discussing the perennially confusing concepts of vector operators and spherical tensors, and use these to give a quick overview of the Wigner–Eckart theorem and selection rules. These latter subjects are then made precise using the notion of a representation operator. We conclude by showing that Dirac’s famous gamma matrices can be understood in terms of representation operators, which then immediately gives the transformation properties of the “Dirac bilinears” of QED.
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Notes
- 1.
Note that the ‘l’ in the superscript of T m (l) is in parentheses; this is because the l isn’t really an active index, but just serves to remind us which SO(3) representation we’re dealing with.
- 2.
These are known as Wigner functions or Wigner D-matrices.
- 3.
References
T. Frankel, The Geometry of Physics, 1st edn. (Cambridge University Press, Cambridge, 1997)
J.J. Sakurai, Modern Quantum Mechanics, 2nd edn. (Addison Wesley Longman, Reading, MA, 1994)
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Jeevanjee, N. (2015). The Representation Operator and Its Applications. In: An Introduction to Tensors and Group Theory for Physicists. Birkhäuser, Cham. https://doi.org/10.1007/978-3-319-14794-9_6
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DOI: https://doi.org/10.1007/978-3-319-14794-9_6
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Publisher Name: Birkhäuser, Cham
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