Unusual spin coupling between Mo
III and Mn
II cyano-bridged ions in bimetallic molecular magnetsbased on the [Mo
III(CN)
7]
4- heptacyanometalate is analyzed in terms of the superexchange theory. Due tothe orbital degeneracy and strong spin-orbit coupling on Mo
III, the ground state of the pentagonal-bipyramidal[Mo
III(CN)
7]
4- complex corresponds to an anisotropic Kramers doublet. Using a specially adapted kineticexchange model we have shown that the Mo
III-CN-Mn
II superexchange interaction is extremelyanisotropic: it is described by an Ising-like spin Hamiltonian
J for the apical pairs and by the
Jz +
Jxy(
+
) spin Hamiltonian for the equatorial pairs (in the latter case
Jz and
Jxy canhave opposite signs). This anisotropy resulted from an interplay of several Ising-like (
) andisotropic (
SMoSMn) ferro- and antiferromagnetic contributions originating from metal-to-metal electron transfersthrough the
and
orbitals of the cyano bridges. The Mo
III-CN-Mn
II exchange anisotropy is distinct fromthe anisotropy of the
g-tensor of [Mo
III(CN)
7]
4-; moreover, there is no correlation between the exchangeanisotropy and
g-tensor anisotropy. We indicate that highly anisotropic spin-spin couplings (such as theIsing-like
J )
combined with large exchange parameters represent a very important source of theglobal magnetic anisotropy of polyatomic molecular magnetic clusters. Since the total spin of such clustersis no longer a good quantum number, the spin spectrum
pattern can differ considerably from the conventionalscheme described by the zero-field splitting of the isotropic spin of the ground state. As a result, the spinreorientation barrier of the magnetic cluster may be considerably larger. This finding opens a new way inthe strategy of designing single-molecule magnets (SMM) with unusually high blocking temperatures. Theuse of orbitally degenerate complexes with a strong spin-orbit coupling (such as [Mo
III(CN)
7]
4- or its 5
dana
logues) as building blocks is therefore very promising for these purposes.