Abstract

The magnetic order-disorder layering transitions of a spin-1 Ising model are investigated, under the effect of a variable surface crystal field Δs\Delta_{s}, using the mean field theory. Each layer kk, of the film formed with NN layers, disorders at a finite surface crystal field distributed according to the law Δk=Δs/kα\Delta_k=\Delta_s/k^\alpha, k=1,2,...,Nk=1,2,...,N and α\alpha being a positive constant. We have established the temperature-crystal field phase diagrams and found a constant tricritical point and a reentrant phenomenon for the first k0k_0 layers. This reentrant phenomenon is absent for the remaining Nk0N-k_0 layers, but the tricritical points subsist and depend not only on the film thickness but also on the exponent α\alpha. On the other hand, the thermal behaviour of the surface magnetisation for a fixed value of the surface crystal field Δs\Delta_{s} and selected values of the parameter α\alpha are established.Comment: 10 Pages Latex, 9 Figures Postscript. To appear in JMMM (2002

    Similar works

    Full text

    thumbnail-image

    Available Versions

    Last time updated on 02/01/2020