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Figure 8.10 Variation of the inverse magnetic
susceptibility with temperature [32] .
Source: Courtesy of the Gauthier-Villars/ESME,
Paris.
2.5
2.0
1.5
1.0
0.5
0.0
0
100
200
300
θ p
T (K)
60 K).
The variation of the inverse magnetic susceptibility with the temperature is given in
Figure 8.10 for BaMn(CO 3 )F 2 .AboveT
Ferromagnetic interactions must also take place at low temperature (T
,
90 K, the linear Curie
Weiss law is well
obeyed, leading to a molar Curie constant C M 5
4.39 (as compared to the theoretical
4.375 for Mn 2 1 ) and a Curie paramagnetic temperature
value C M 5
θ p 52
52 K.
This value of
θ p , together with the deviation of 1/x from the Curie
Weiss law at
T
90 K indicates that antiferromagnetic interactions dominate; however, no clear
evidence of magnetic order can be found at a low temperature [32] .
Magnetic susceptibility of Mn 2 PO 4 F and CO 2 PO 4 F has been studied by Leblanc
et al. [33] . The variation of the inverse magnetic susceptibility Xg 2 1 with tempera-
ture ( Figure 8.11 ) and the absence of field dependence of the susceptibility are
indicative of antiferromagnetic behavior with T N 5
,
14 K for Mn 2 PO 4 F
and CO 2 PO 4 F, respectively. Above approximately 100 K, the Curie
15 and T N 5
Weiss law is
well obeyed and yields
θ p 52
50 K, C M 5
8.2 and
θ p 52
53 K, C M 5
6.4. These
molar Curie constants, which give
μ eff 5
5.70 and 5.1
μ B , are in good agreement
8.75 (spin only value) for Mn 2 1 and with the
with the calculated value C M (th)
5
value usually found for CO 2 1 .
8.7 Hydrothermal Synthesis of Tungstates
Tungstates form an important class of materials with a wide range of divalent and
trivalent metals in their composition. Among the trivalent metals, the rare earth and
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