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References for Chapter 12
See B. T. Feld, Models of Elementary Particles, Blaisdell, Waltham (1969), Fig. 16.6 on page 382.
Particle Data Group, “Review of Particle Properties”, Rev. Mod. Phys. 48, No. 2, Part II, April (1976). The “well-established” states have *** and **** ratings.
The broad-width Ξ resonances are not well-enough established to include in Fig. 12.4.
For an early discussion of these baryon rotations, see M. H. Mac Gregor, Lett. Nuovo Cimento 1, 427 (1971).
S. A. Moszkowski, Handbüch der Physik, Vol. 34, Berlin (1957), p. 413, Eq. 36.3.
A. Bohr and B. Mottelson, Kgl. Danske Videnskab Selskab Mat. fys. Medd. 27, No. 16 (1953); J. P. Davidson, Collective Models of the Nucleus, New York (1968).
Z. Szymanski, Trieste Lectures, Vienna (1970), p. 67.
Ref. 7, p. 94.
Ref. 7, p. 101.
See, for example, A. K. Kerman, Nuclear Reactions, edited by P. M. Endt and M. Demeur, Amsterdam (1959), Chapter X.
S. A. Moszkowski,Handbüch der Physik, Vol. (1957), p. 483.
See the U238 spectrum in Fig. 7.1 of Ref. 7. Note that for vibrational modes with S ≠ 0, all successive values of ℓ appear.
S. A. Moszkowski, Handbüch der Physik, Vol. (1957), p. 495.
See M. H. Mac Gregor, Phys. Rev. D9, 1259 (1974), Ref. 150.
See Ref. 151 in Ref. 14.
See Ref. 152 in Ref. 14.
See Ref. 153 in Ref. 14.
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(1978). Spin and orbital angular momentum components of baryons. In: The Nature of the Elementary Particle. Lecture Notes in Physics, vol 81. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-08857-1_15
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