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D. Kerlick, and J. M. Nester, "General Relativity with Spin and Torsion: Foundations and Prospects," Rev. Mod. Phys. 48 (1976), 393-416. 19 E. B. Dynkin, "Semisimple Subalgebras of Semisimple Lie Algebras," Ann. Math. Soc. Transl. (Ser. 2) 6 (1957), 111-244; E. B. Dynkin, "Maximal Subgroups of the Classical Groups," Ann. Math. Soc. Transl. (Ser. 2) 6 (1957), 245-379; E. B. Dynkin, Usp. Mat. 4(1947), 59-127. 20 Y. Ne'eman, "Derivation of Strong Interactions from a Gauge Invariance," Nucl. Phys. 26 (1961), 222-9; "Yukawa Terms in the Unitary Gauge Theory," Nucl.
D. Linde, Inflation and Quantum Cosmology, Academic Press, Boston (1990). E. Harrison, Phys. Rev. D l (1970) 2726; see ref. 26 there. Y. , "Nuclear Physics Implication of the Spin 2 Multiplet", Symmetry Principles at High Energy, (Proc. of the Fifth Coral Gables Conf. (1968)), W. A. Benjamin, NewYork (1968), pp. 149-151. Y. , "Renewal of the Astronomical Research in Eretz- Israel (25 Years of the Florence and George Wise Observatory) (Hebrew) Bull. Israel Acad. Sci. of Humanities 2 (Feb. 1997) 8.
Gell-Mann had circulated a first draft at Caltech on 20 January. He submitted a second version to the Physical Review on 27 March, then withdrew it in June when E-A relative-parity measurements appeared to invalidate the octet assignments. 22 The Sakata model and the octet are introduced as two candidate realizations of SU(3). Gell-Mann's method of "current algebra" was an important step in providing a justification for strong-interaction symmetries, even if one had to abandon RQFT, following the criticism and advice from the Berkeley S- 29 The classification and structure ofhadrons 635 matrix school.