Abstract
The simple model of a classical spin-glass proposed by van Hemmen [1] is extended to the case of a generalS Ising spin and anisotropy energy. Due to its simplicity, the model is amenable to an exact solution and in the case of spin-1 the phase diagram is similar to that of the Sherrington-Kirkpatrick model. ForS=1 and for certain values of the anisotropy the phase diagram in the (H-T) plane shows continuous and discontinuous transitions, a critical point within the condensed phase, and a field-induced mixed phase in addition to the paramagnetic and spin-glass phases.
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References
Hemmen, J.L. van: Phys. Rev. Lett.49, 409 (1982)
Hemmen, J.L. van, Enter, A.C.D. van, Canisius, J.: Z. Phys. B-Condensed Matter50, 311 (1983)
Sherrington, D., Kirkpatrick, S.: Phys. Rev. Lett.35, 1792 (1975)
Choy, T.C., Sherrington, D.: J. Phys. C17, 739 (1984)
Hopfield, J.J.: Proc. Natl. Acad. Sci. USA79, 2554 (1982)
Ghatak, S.K., Sherrington, D.: J. Phys. C10, 3149 (1977)
Lage, E.J.S., Almeida, J.R.L. de: J. Phys. C15, L1187 (1982)
Mottishaw, P.J., Sherrington, D.: J. Phys. C18, 5201 (1985)
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de Almeida, J.R.L., Brady Moreira, F.G. Magnetic field effects on a classical anisotropic spin-glass model. Z. Physik B - Condensed Matter 63, 365–367 (1986). https://doi.org/10.1007/BF01303816
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DOI: https://doi.org/10.1007/BF01303816