We consider here the masses, decay rates, and decay spectra of the octet of 0^- mesons, the nonet of 1^- mesons, the $X(960)$ resonance, and a proposed η*(1620) resonance having the quantum numbers of η(550). We use spin-unitary-spin symmetry and nonet symmetry, so that the mesons fall into 36 states, combining an SU(6)1, with an SU(6)35. Further, we fix the strength of the couplings of the SU(3) octets in the 36 with respect to the SU(3) singlets by assuming that the form of the coupling remains unchanged when we include the singlet states. We are then able---after making a particular choice of Hamiltonion---to predict the masses M_η*,M_ρ^±,M_ρ⁰,M_K^*±,M_K*0 and the decay rates Γ_ω→π⁺π^-, Γ_φ→π⁺π^-, Γ_φ→π⁺π^-π⁰, using as input the masses of the octet of 0^- mesons and M_φ,M_ω. These predictions are in reasonable agreement with presently existing experimental data. We further discuss related meson decays using the above scheme to eliminate the arbitrariness in the relative coupling strength of the singlet states. Specifically we consider V→P+P^', V→3P, V→P+γ, V→P+P^'+γ [discussing C noninvariance and S-wave pion-pion resonances and their effect in (ω,φ)→π⁺π^-γ, V→l⁺+l^-, P→2γ, P→P^'+P^''+γ, and P→l⁺+l^-+γ. We use the model of Gell-Mann, Sharp, and Wagner and give invariant-mass spectra for the three-body decays.
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Joel Yellin (1966) studied this question.
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