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 Σ hyperons determined from the mass differences of Σ and the mirror theorem are compared with the perturbation results.

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