The magnetic order-disorder layering transitions of a spin-1 Ising model are
investigated, under the effect of a variable surface crystal field
Δs, using the mean field theory. Each layer k, of the film formed
with N layers, disorders at a finite surface crystal field distributed
according to the law Δk=Δs/kα, k=1,2,...,N and α
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 k0 layers. This reentrant phenomenon is absent for
the remaining N−k0 layers, but the tricritical points subsist and depend
not only on the film thickness but also on the exponent α. On the other
hand, the thermal behaviour of the surface magnetisation for a fixed value of
the surface crystal field Δs and selected values of the parameter
α are established.Comment: 10 Pages Latex, 9 Figures Postscript. To appear in JMMM (2002