Abstract

We present Molecular Dynamics simulation results for confined ferromagnetic nanoparticles (film geometry) under the influence of strong, homogeneous magnetic fields. We focus on the role of short-ranged attractive interactions between the particles for the structure formation in thin films consisting of four to five monolayers. To this end we compare simulation results for Stockmayer particles (Lennard-Jones plus dipolar interactions) with corresponding results for dipolar soft spheres, where the short-ranged potential is purely repulsive. At moderate and large average densities, both systems exhibit pronounced layering. Based on the corresponding normal pressure oscillations we show that the field-induced effects on the layer formation in this density range are essentially independent of the short-range interactions. The dipolar soft sphere system merely has a stronger tendency to form a crystal-like lateral structure upon application of a parallel field. More pronounced differences occur at lower densities and not too high dipolar coupling strengths within the vapour–liquid region of the confined, zero-field Stockmayer system. Applying a perpendicular field, the Stockmayer system develops a blob structure absent in the corresponding repulsive system. Finally, for very large values of both, dipolar coupling parameter and field strength of a perpendicular field, we find evidence for a field-induced in-plane crystallisation of the layered systems.

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