“…By dω we denote the surface element on the sphere Ω R . The non-uniqueness of recovering a vertically integrated magnetization m from the knowledge of V in Ω ext R can be characterized by a fairly well-known decomposition (see, e.g., [1,8,11,12,13,18,19,22]) m =m (1) +m (2) +m (3) , (1.3) which has the property that V ≡ 0 in Ω ext R if and only ifm (2) ≡ 0 (in other words, any magnetization of the form m =m (1) +m (3) produces no magnetic potential in the exterior Ω ext R ). We call such a decomposition a Hardy-Hodge decomposition (cf.…”