Relativistic corrections to magnetic dipole moments

Relativistic corrections to magnetic dipole moments of odd nuclei (208Pb ± one particle) are calculated using the self-consistent Dirac-Hartree equations. The contributions of nuclear core polarization are taken into account within the framework of the theory of finite Fermi systems. In contrast to light nuclei, relativistic corrections have reasonable values for odd neighbors of 208Pb. Relativistic effects show a weak dependence on small variations of effective fields in the Dirac-Hartree equations. Polarization contributions are sensitive to the choice of constants for the amplitude of spin-spin nucleon interactions. 7 refs., 2 tabs