Abstract
In \(SU\left( 2\right) \), the charge operator is:
\(\displaystyle Q=eT_3=\frac 12\left( \begin{array}{cc} e & 0 \\ 0 & -e \end{array} \right) ~~~~~~~{\rm (D.1)}\)
The quarks form a doublet in the fundamental representation of \(SU\left( 2\right) \):
\(\displaystyle q=\left( \begin{array}{c} q_R \\ q_B \end{array} \right) \;\;\;\;\;\;Q\left( \begin{array}{c} q_R \\ q_B \end{array} \right) =\frac 12e\left( \begin{array}{c} q_R \\ -q_B \end{array} \right)~~~~~~~{\rm (D.2)}\)
The red and blue quarks have respectively color charges \(\frac 12e\) and \(-\frac 12e\).
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Ripka, G. Appendix D. Color Charges of Quarks and Gluons. 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_9
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DOI: https://doi.org/10.1007/978-3-540-40989-2_9
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