Abstract
The three Pauli matrices are:
\(\displaystyle \sigma ^1=\left( \begin{array}{ll} 0 & 1 \\ 1 & 0 \end{array} \right) \;\;\;\;\;\;\sigma ^2=\left( \begin{array}{ll} 0 & -i \\ i & 0 \end{array} \right) \;\;\;\;\;\;\sigma ^3=\left( \begin{array}{ll} 1 & 0 \\ 0 & -1 \end{array} \right)~~~~~~{\rm (C.1)} \)
\(\displaystyle \sigma _i\sigma _j=\delta _{ij}+i\varepsilon _{ijk}\sigma _k~~~~~~{\rm (C.2)} \)
The three generators of the \(SU\left( 2\right) \) group are \(T_a=\frac 12\sigma _a\).
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Ripka, G. Appendix C: The Generators of the SU(2) and SU(3) Groups. In: Ripka, G. (eds) Dual Superconductor Models of Color Confinement. Lecture Notes in Physics, vol 639. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-40989-2_8
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DOI: https://doi.org/10.1007/978-3-540-40989-2_8
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