We use a simple van der Waals theory, suitably extended to the solid phase and to anisotropic interactions, to study the phase behavior of a system of particles with magnetic exchange interactions. A very rich phase behavior is found which indicates, in particular, that the ferromagnetic liquid phase is favored by increasing the range of both the magnetic exchange interactions and of the nonmagnetic interactions. This could well explain why it turns out to be difficult to find such a phase in simulations which use interactions which are cut off at finite range.
It is shown that the region of the phase diagram where the ferromagnetic liquid phase of a Heisenberg fluid (with long-ranged exchange interactions) is thermodynamically stable (relative to the solid phases) remains confined to a fairly small temperature–density domain also in the presence of nematic interactions. The present analysis is carried out on the basis of a van der Waals theory for both translationally and/or orientationally ordered and disordered phases.
We develop the calculation of free energy in a nematic phase for a model of spherical particles with the long-range anisotropic interaction from the van der Waals theory. We map the gas-liquid equilibrium, which is coupled to a first-order isotropic-nematic transition. We discus how the topology of the phase diagrams changes upon varying the strengths of the isotropic and nematic interactions.
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