The magnetic behavior of nanocrystalline alloys has been modeled using atomic Monte Carlo simulation. The model consists of a cubic lattice composed of a ferromagnetic nanograin in a ferromagnetic matrix. The magnetizations of nanograin core, surface and interface regions and matrix were studied as a function of the exchange coupling between the nanograin and the matrix, as well as of the nanograin/matrix volume ratio, equivalent to the crystalline fraction in the nanocrystalline alloys. The mechanism of polarization of the matrix by fields penetrating from the nanograin is discussed and correlated with the matrix–nanograin exchange coupling. Competition between interface anisotropy and magnetocrystalline anisotropy produces spin-glass-like magnetic order of the interfacial regions.

1.
G. Herzer, Handbook of Magnetic Materials, edited by K. H. J. Buschow (Elsevier, New York, 1997), Vol. 10.
2.
A.
Slawska-Waniewska
and
J. M.
Grenèche
,
Phys. Rev. B
56
,
R8491
(
1997
).
3.
A.
Hernando
and
T.
Kulik
,
Phys. Rev. B
49
,
7064
(
1994
).
4.
I.
Navarro
,
M.
Ortuno
, and
A.
Hernando
,
Phys. Rev. B
53
,
11656
(
1996
).
5.
J. S.
Garitaonandia
,
D. S.
Schmool
, and
J. M.
Barandiaran
,
Phys. Rev. B
58
,
12147
(
1998
).
6.
J. M.
Grenèche
,
M.
Miglierini
, and
A.
Slawska-Waniewska
,
Hyperfine Interact.
126
,
27
(
2000
).
7.
K. Binder and D. W. Heermann, Monte Carlo Simulation in Statistical Physics (Springer, Berlin, 1992).
8.
O. Crisan, Y. Labaye, L. Berger, and J. M. Greneche (to be published).
9.
A.
Hernando
,
J. Phys.: Condens. Matter
11
,
9455
(
1999
).
10.
J.
Skorvanek
,
J.
Kovac
, and
J. M.
Grenèche
,
J. Phys.: Condens. Matter
12
,
9085
(
2000
).
11.
Y.
Labaye
,
O.
Crisan
,
L.
Berger
,
J. M.
Grenèche
, and
J. M. D.
Coey
,
J. Appl. Phys.
91
,
8715
(
2002
).
This content is only available via PDF.
You do not currently have access to this content.