Prog. Theor. Phys. Vol. 32 No. 6 (1964) pp. 981-982

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Internal Space of Baryons and Mesons

Department of Physics, Nagoya University, Nagoya

(Received September 28, 1964)

URL : http://ptp.ipap.jp/link?PTP/32/981/
DOI : 10.1143/PTP.32.981

The present model is the extention of the simpler ones as given in T. Takabayasi, Nuovo Cim. 23 (1962), 222; ibid. 28 (1963), 184.
For an oscillator model for particles which introduces internal degrees within the Lorentz space, see T. Takabayasi, Nuovo Cim. 33 (1964), 668;
cf. H. Yukawa, Prog. Theor. Phys. 31 (1964), 1167[PTP];
Y. Katayama and H. Yukawa, Prog. Theor. Phys. 32 (1964), 366[PTP];
Y. Katayama, Prog. Theor. Phys. 32 (1964), 368[PTP].
Clearly b_i^*b_j^*b_k^*|>0 gives 10^*.
Mathematically SU₃ eigenfunctions may also be obteined in a different parametrization as shown, e.g. by Y. Ohnuki (private communication).
cf. T. Takabayasi, Nuovo Cim. 33 (1964), 668; Prog. Theor. Phys. 31 (1964), 1180[PTP].
Symmetry-breaking adds to (4) the term -bY+c{T²-Y²/4-[K²+KL+L²+3(K+L)]/9}.

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