Abstract
According to the theory of d'Espagnat and Prentki the anomalous magnetic moments of hyperons are calculated in the lowest-order perturbation approximation. It is further shown that their charge-independent interaction Hamiltonian leads to the mirror theorem for the anomalous magnetic moments of baryons (and of K mesons) without use of perturbation approximation. Finally the anomalous magnetic moments of SIGMA hyperons determined from the mass differences of SIGMA and the mirror theorem are compared with the perturbation results. (auth)
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