1Polymer Physics and Critical Phenomena Laboratory, Faculty of Sciences Ben M’sik, Hassan II University of Casablanca, P. O. Box 7955, Casablanca, Morocco
International Journal of Physics.
2018,
Vol. 6 No. 4, 116-121
DOI: 10.12691/ijp-6-4-3
Copyright © 2018 Science and Education PublishingCite this paper: A. Waddahou, M. Chahid, A. Maârouf, F. Benzouine. Critical Behavior at Surfaces of Strong Coupling Paramagnetic Systems Exhibiting a Paramagnetic-Ferrimagnetic Transition.
International Journal of Physics. 2018; 6(4):116-121. doi: 10.12691/ijp-6-4-3.
Correspondence to: M. Chahid, Polymer Physics and Critical Phenomena Laboratory, Faculty of Sciences Ben M’sik, Hassan II University of Casablanca, P. O. Box 7955, Casablanca, Morocco. Email:
mustapha.chahid@gmail.comAbstract
The purpose of this work is the investigation of the critical surface effects of two strongly coupled paramagnetic sublattices exhibiting a para-ferrimagnetic transition. The model is of Landau-Ginzburg type, whose bulk free energy is a functional of two kind of order parameters (local magnetizations) φ and

This free energy involves, beside quadratic and quartic terms in both φ and

, a lowest-order coupling,

where C
o<0 is the coupling constant measuring the interaction between the two sublattices. Two terms Hφ and

are also introduced, to describe the interaction within an external magnetic field
H. We introduce a surface free energy expanded in terms of the local order parameters. The magnetization at the surface are φ
s and

We show, in particular, that the model can be reduced to an effective theory written in terms of the overall magnetization

and the associated fraction of magnetization

. This formulation leads us to define an effective extrapolation length λ
s. We then derive all the critical properties of the system close to the critical temperature
Tc. In particular, we determine the critical behavior of the overall surface magnetization

, in terms of
b above and below
Tc. The variations of
s with the magnetic field
H, and when a surface field H
s is applied actually at
Tc, are derived. We determine, also, the associated susceptibilities at the surface χ
s and χ
s.s. The determination of the full profile of the magnetization close to the surface will be the subject of a future communication.
Keywords