Journal of Magnetism and Magnetic Materials 70 (1987) 345-346 345
North-Holland, Amsterdam
MAGNETIC PROPERTIES OF (GdxY t_ x)Co4B COMPOUNDS
E. BURZO and M. URSU
Central Institute of Physics, P.O. Box MG-6, Bucharest, Romania
The magnetic properties of (Gd,Y I ~)Co4B compounds were studied in the temperature range 4.2-1000 K. The
compounds with x/> 0.2 are ferrimagnetically ordered. The mean cobalt moment increases from 0.67~, in YCo4B to 0.98p.~
in GdCo4B. The temperature dependence of the reciprocal susceptibilities for compounds with x >/0.2 may be described by a
hyperbolic law of N6el-type.
The RCo 4B compounds, where R is a rare earth
or yttrium, crystallize in CeC%B-type structure
[1]. This is obtained by ordered substitutions of
cobalt by boron in every second layer of CaCu 5-
structure. The cobalt atoms occupy two types of
sites. The magnetic properties of RCo4B com-
pounds were reported by Oesterreicher et al. [2]
and Pedziwiatr et al. [3]. The GdCo4B is ferri-
magnetically ordered while in case of YCo4B a
ferromagnetic ordering is evidenced.
In order to obtain information of the magnetic
behaviour of cobalt in compounds with CeC%B-
type structure, we studied the (Gd~YI_~)Co4B
system. In this system the electron concentration
is not modified by the gradual substitution of
yttrium by gadolinium. Thus, the variation of
cobalt moment may be attributed only to the
changes in the magnetic interactions involving the
cobalt atoms.
The (Gd,Y 1 .x)Co4B compounds were prepared
by melting the constituent elements in a water-
cooled copper boat by rf heating under argon
atmosphere. The compounds were annealed for
one week at 900°C and then rapidly cooled to
room temperature. The X-ray analysis showed the
presence of only one phase. Magnetic measure-
ments were performed by means of several types
of equipment, in the temperature range 4.2-1000
K.
In analysing the data we use a two sublattice
model corresponding to gadolinium and cobalt
magnetizations.
The composition dependence of the magnetiza-
tions is plotted in fig. la. The magnetizations of
the gadolinium and cobalt sublattices are com-
pensated for x = 0.47. Supposing that the mag-
netic moment of gadolinium is 7/~B, we determined
the cobalt contribution to the magnetization - fig.
lb. The cobalt moment is dependent on composi-
tion increasing from 0.67/x B (x = 0) up to 0.98/~ B
(x = 1.0).
The ferrimagnetic ordering evidenced by
saturation studies for compounds having x >~ 0.2
is also proved by magnetic measurements above
the Curie points. As seen in fig. 2, the inverse of
the paramagnetic susceptibility as function of tem-
perature follows a hyperbolic law of N6el-type,
which can be expressed in the form [4]
--1 1 l l
X =Xo +TC -o(T-O) (1)
We denoted by C the Curie constant and by
X0, o and 0 the parameters which are functions of
the molecular field coefficients.
According to the addition law of susceptibilities
and supposing that the Curie constant of
z 25
_>'~ N
02 04 06 08 1.0
~ COMPOSfTION { x)
The composition dependence of the saturation magneti-
(a), cobalt magnetization (b) and the effective cobalt
moments (c).
Fig. 1.
zation
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