Two types of magnetic dipole fields are generated by thermal convection in
a rotating spherical shell. The axial (or equatorial) dipole in which the m
agnetic dipole moment is parallel (or perpendicular) to the rotation axis i
s realized at a larger (or smaller) value of the Rayleigh number. Their str
ucture is robust and persists over the entire simulation period, that is, e
ight (or two) magnetic diffusion times.