In the Pauli-Dirac representation of Table 14.1, a suitable charge conjugation operator is (C=i gamma^{2} gamma^{0}). Show
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In the Pauli-Dirac representation of Table 14.1, a suitable charge conjugation operator is \(C=i \gamma^{2} \gamma^{0}\). Show that \(C\) is given explicitly by the matrix
in this representation. Verify by matrix multiplication the matrices for \(\gamma^{5}\) shown in Table 14.1 for the Pauli-Dirac and Weyl (chiral) representations. Hint: A useful identity for Pauli matrices is \(\sigma_{1} \sigma_{2} \sigma_{3}=i \mathrm{I}^{(2)}\), where \(\mathrm{I}^{(2)}\) is the \(2 \times 2\) unit matrix.
Data from Table 14.1
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Related Book For
Symmetry Broken Symmetry And Topology In Modern Physics A First Course
ISBN: 9781316518618
1st Edition
Authors: Mike Guidry, Yang Sun
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