Spin-dependent quark-quark interaction and baryon magnetic moments

The magnetic moments of the baryons belonging to the low-lying SU(3) octet are computed using second-order perturbation theory taking into account the effect of the spin-dependent interactions that are expected to arise in quantum chromodynamics. The unperturbed eigenfunctions of the confining Hamiltonian are approximated by harmonic-oscillator wave functions, and the flavor X spin parts belong, in the limit of equal quark masses, to irreducible representations of SU(6). In this basis we then calculate the mixing of the (56, $0^{+}$) ground-state wave function with the orbital and radial excitations labeled by (56, $0_R^{+}$), (70, $0^{+}$), (20, $1^{+}$), and (70, $2^{+}$). This mixing arises not only from the spin-dependent interactions but also from the differences among quark masses. Finally we comment on the contributions to the magnetic moments not taken into account in this work.