We find three unanticipated features in the magnetic response of dilute systems of highly monodisperse Fe nanoparticles. Above a spin freezing temperature (Tf) the remanent magnetization relaxes smoothly to zero, but below Tf the relaxation halts abruptly at a nonzero value. The distribution of relaxation rates changes at a percolation temperature (Tₚ), consistent with chainlike structures above Tₚ and three-dimensional clusters below Tₚ. The blocking temperature (Tb) varies inversely proportional to particle diameter, opposite to the behavior of the N\'eel-Brown model for individual domains, but consistent with a type of Casimir-Polder interaction expected between dilute nanometer-scale particles.
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Chamberlin et al. (2002) studied this question.
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