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A calculation of SU(4) Clebsch–Gordan coefficients
1.For a comprehensive review of SU(4) and SU(8) schemes of hadron physics, see: J. W. Moffat, “SU(4) and the New Hadrons,” lectures at the McGill Summer School of Physics, June 1975 [to appear in Proceedings of the McGill Summer School of Physics, June 1975 (to be published)].
2.G. S. Abrams, invited talk at the SLAC Symposium on Electron—Photon Interactions, August, 1975 (to be published in Proceedings of the SLAC Symposium on Electron—Photon Interactions, August, 1975).
3.J. D. Bjφrken and S. L. Glashow, Phys. Lett. 11, 255 (1964).
4.V. Rabl, G. Campbell Jr., and K. C. Wali, J. Math. Phys. 16, 2494 (1975).
5.D. Amati, H. Bacry, J. Nuyts, and J. Prentki, Nuovo Cimento 34, 1732 (1964). In this paper, the in the expansion of should read whereas the in should read
6.In Ref. 5, the SU(3) content of SU(4) representations up to are given. Note that the representation 60 contains a 15 and a not a and a 6, at
7.L. C. Biedenharn, J. Math. Phys. 4, 436 (1963);
7.G. E. Baird and L. C. Biedenharn, 4, 1449 (1963); , J. Math. Phys.
7.G. E. Baird and L. C. Biedenharn, 5, 1723, 1730 (1964)., J. Math. Phys.
8.J. W. Moffat, Phys. Rev. 140, B1681 (1965).
9.S. L. Glashow, J. Iliopoulos, and L. Maiani, Phys. Rev. D 2, 1285 (1970).
10.J. W. Moffat, Phys. Rev. D 12, 286, 288 (1975).
11.S. Okubo, Phys. Rev. D 11, 3261 (1975).
12.J. J. de Swart, Rev. Mod. Phys. 35, 916 (1963).
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