Abstract
For a long time considerable litterature has been devoted to one-dimensional spin systems. The possibility of exactly solving various non trivial cases has been a strong motivation in this field. More recently the increasing number of new compounds showing quasi one-dimensional magnetic behavior gave a further impulsion to this subject. In the past, mainly so-called ferromagnetic and antiferromagnetic chains were considered from the point of view of their static properties1. Then, dynamic properties were considered2, and later on much attention was paid to ferrimagnetic chains,3 showing two types of alternating cations. A large variety of situations are involved in this last category, giving rise to new specific problems4. In the present article we are concerned with the static magnetic properties of a large class of ferrimagnetic chains defined by the following two conditions:-i) Two types of cations alternate along the chain. One of them, at least, must be characterized by a spin number large enough to be treated classically; ii) The hamiltonian is fully isotropic (Heisenberg coupling, no spin-lattice anisotropy) within the spin space.
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Curély, J. et al. (1987). Magnetism of Quantum-Classical Ferrimagnetic Chains Showing Alternate Heisenberg Coupling: Application to MnCu (Obp)(H2O)3, H2O. In: Delhaes, P., Drillon, M. (eds) Organic and Inorganic Low-Dimensional Crystalline Materials. NATO ASI Series, vol 168. Springer, New York, NY. https://doi.org/10.1007/978-1-4899-2091-1_49
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DOI: https://doi.org/10.1007/978-1-4899-2091-1_49
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