Abstract
Abstract Hysteresis curves of molecular nanomagnets display a step-like behavior typical of the relaxation through quantum tunneling of the magnetization. The relaxation rate depends on the value of the so-called tunnel splitting, i.e., the gap between quasi-degenerate states in correspondence of a level anticrossing. In the case of Fe 8 , the magnitude of this gap deduced by Landau–Zener measurements seems incompatible with the value calculated by using the Hamiltonian determined by spectroscopic measurements. We show that the commonly neglected quantum fluctuations of the magnitude of the total spin of the molecule ( S mixing) hugely affect the tunnel splitting, and allow the above-mentioned discrepancy to be solved. Since the degree of S mixing is strongly influenced by the topology of the molecule, we suggest that cluster topology is one of the key ingredients in designing new nanomagnets.
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