Author:
Glashow S. L.,Sakurai J. J.
Publisher
Springer Science and Business Media LLC
Subject
Astronomy and Astrophysics,Nuclear and High Energy Physics,Atomic and Molecular Physics, and Optics
Reference8 articles.
1. S. L. Glashow andJ. J. Sakurai:Nuovo Cimento,25, 337 (1962). See especially the Appendix. In this reference, we stressed the representation 27 rather than the 10 partly because we wished to include both the Y 1 * (1385 MeV) and the Y 0 * (1405 MeV) in the sameJ = 3/2 + unitary supermultiplet. Now that the Y 0 * seems to be an s-wave KN bound state of the Dalitz-Tuan type [seee.g.,T. Akiba andR. H. Capps:Phys. Rev. Lett.,8, 457 (1962)], the representation 27 is no longer so appealing.
2. S. Okubo:Prog. Theor. Phys.,27, 949 (1962). This formula is a generalization of the mass formula for the octet first derived byM. Gbll-Manx:Phis. Rev.,125, 1067 (1962).
3. L. Bertanza:Proceedings of the 1962 International Conference on High Energy Physics at CERN (to be published).
4. H. Ticho:Proceedings of the 1962 International Conference on High Energy Physics at CERN (to be published).
5. M. Gell-Mann:Proceedings of the 1962 International Conference on High Energy Physics ai CERN (to bo published). This « equal-spacing rule» applies to all multiplets of SU(3) belonging to representations with only upper (or lower) indices, like the 10. SeeS. L. Glashow:International Summer School on Group Theoretic Methods in Elementary Particle Physics at Istanbul 1962 (to be published).
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