Publisher
Springer Berlin Heidelberg
Reference40 articles.
1. See the lecture by Barut, A. O.: Springer Tracts in Mod. Phys., Vol. 50 (1969).
2. Kleinert, H.: Fortschr. Phys. 16, 1 (1968).
3. For an extensive study of this subject see: Hamprecht, B., and H. Kleinert: Univ. of Colorado preprint, May 1968; Hamprecht, B.: Fortschr. Phys. 16, 35 (1969). There are very few parameters in this approach reproducing the decay properties of almost the complete Rosenfeld table for baryon resonances.
4. Kleinert, H.: Phys. Rev. 163, 1807 (1967). Kleinert, H., Barut, A. O., D. Corrigan, and H. Kleinert: Phys. Rev. Letters 20, 167 (1968). Kleinert, H. Corrigan, D.: University of Colorado, Thesis (1968). In particular, the theory is able to reproduce the experimentally observed double pole formula for G
E
P
=G
M
P
/μ
P
=G
M
n
/μ
n
and
$$G_E^n = \frac{t}{{4m^2 }}G_M^n $$
.
5. -: Phys. Rev. Letters
18, 1027 (1967). One simply assumes the pseudoscalar to transform as an octet operator under SU (3) and uses experimental masses. The mass splitting cause SU (3) breaking in the form factors. Only the unphysical transitions at rest are SU (3) symmetric.
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