@article{ijp2018652,
author={{Waddahou, A. and Chahid, M. and Maarouf, A.},
title={Order Parameter Profiles near Surfaces of Super-weak Ferrimagnetic Materials Exhibiting a Paramagnetic-Ferrimagnetic Transition},
journal={International Journal of Physics},
volume={6},
number={5},
pages={147--154},
year={2018},
url={http://pubs.sciepub.com/ijp/6/5/2},
issn={2333-4576},
abstract={The aim of this paper is to determine the full order parameter profiles close to the surface for a system made of two strongly coupled paramagnetic sublattices of respective moments &#966; and &#968;. The material exhibits a para-ferrimagnetic transition at some critical temperature <i>T</i><SUB><i>c</i></SUB> greater than the room temperature. The free energy describing the physics of the system is of Landau type, and involves, beside quadratic and quartic terms in both &#966; and &#968;, a lowest-order coupling, -<i>C</i><SUB><i>o</i></SUB>&#966;&#968; where <i>C</i><SUB>o</SUB>&lt;0 is the coupling constant measuring the interaction between the two sublattices. We consider here below a film of thickness <i>L</i>, and the free energy is then a sum of bulk and surface contributions expanded in terms of the local order parameters. The magnetization at the surface are &#966;<SUB><i>s</i></SUB> and &#968;<SUB><i>s</i></SUB>. As in a recent paper (whom the present work is an extension), we first reduce the model to an effective &#966;<SUP>4</SUP> -theory written in terms of the overall magnetization <img src=image/abs1.png></img> =&#966;+&#968; and the associated fraction of magnetization &#951;<SUB><i>a</i></SUB>=&#966;/(&#966;+&#968;). For the ordinary transition where the extrapolation length is positive &#955;<SUB>s</SUB>>0, we determine the order parameter profile near surfaces. We show, in particular, that the magnetization behavior is governed, in addition of &#955;<SUB>s</SUB> and the bulk correlation length &#958;<SUB>b</SUB><SUP>-</SUP>, by a new length <i>L</i><SUB><i>a</i></SUB>. We have interpreted this latter as the width of the ordered ferrimagnetic layer close to the surface. Finally, we examine the extraordinary (&#955;<SUB>s</SUB>&lt;0), special (&#955;<SUB>s</SUB>=&#8734;) and surface (at <i>T</i><SUB><i>cs</i></SUB>><i>T</i><SUB><i>c</i></SUB>) transitions.},
doi={10.12691/ijp-6-5-2}
publisher={Science and Education Publishing}
}
