References
M. H. Mac Gregor:Lett. Nuovo Cimento,4 1249 (1970).
M. H. Mac Gregor:Lett. Nuovo Cimento,4, 1043 (1970).
M. H. Mac Gregor:Lett. Nuovo Cimento,1 427 (1971).
B. A. Shahbazian: presented atXV International Conference on High-Energy Physics, Kiev, USSR, Aug. 26-Sept. 4, 1970. A review paper from the Kievs Conference,N. P. Samios:Strange bayron resonances, BNL-15284, shows the Shahbazian data in Fig. 14.
Discussion byN. P. Samios in ref. (4).
M. Roos, C. Bricman, A. Barbaro-Galtieri, L. R. Price, A. Rittenberg, A. H. Rosenfeld, N. Barash-Schmidt, P. Söding, Chih Yung Chien, C. G. Wohl andT. Lasinski:Phys. Lett.,33B, 1 (1970). Page 103 of this reference discusses the λ(1327) resonance. See also the January (1969)Review of particle properties (Rev. Mod. Phys.,41, 109 (1969)).
M. H. Mac Gregor:Lett. Nuovo Cimento,4 1309 (1970).
L. J. Gutay et al.: Rotation invariance and the structure of the S-wave ππ cross-section, COO-1428-174, Feb. 1970, submitted for publication.
See the summary of A2 experiments in ref. (6). The A2 dip shown in Fig. 3 is a dipole fit to the neutral A2, as measured by theBCS Collaboration:Lett. Nuovo Cimento,4, 838 (1970).
H. L. Anderson, S. Fukui, D. Kessler, K. A. Klare, M. V. Sherbrook, H. J. Evans, R. L. Martin, E. P. Hincks, N. K. Sherman andP. I. P. Kalmus:Phys. Rev. Lett.,18, 89, (1967).
H. Brody, E. Groves, R. Van Berg, W. Wales, B. Maglic, J. Norem, J. Oostens, G. B. Cvijanovich andR. A. Schluter:Phys. Rev. Lett.,24, 948 (1970).
The rotational level at 525 MeV is the resonance denoted as G2 in ref.(1). A list of experiments in which it has been observed is given in ref. (7)M. H. Mac Gregor:Lett.Nuovo Cimento 4, 1309 (1970).
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Gregor, M.H.M. Evidence for linear meson systematics with baryon numberN=2. Lett. Nuovo Cimento 1, 437–441 (1971). https://doi.org/10.1007/BF02785172
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DOI: https://doi.org/10.1007/BF02785172