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Developments in Ceramic Materials Research

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Synthesis, Spectroscopic and Magnetic Studies… 117<br />

The magnetization vs. field curves registered above (10 K) and below (5 K) the order<strong>in</strong>g<br />

temperature is apparently not too much different but two important po<strong>in</strong>ts must be notice. In<br />

both cases the magnetization curves are nearly l<strong>in</strong>eal up to 7 T, but at lower temperatures a<br />

small change on the slope is observed at about 0.04 T (<strong>in</strong>set <strong>in</strong> Figure 14). Moreover, a weak<br />

magnetization (about 50 cm 3 Oe/mol) is reta<strong>in</strong>ed at zero field. Tak<strong>in</strong>g <strong>in</strong>to account these<br />

results, we performed magnetization measurements vs. temperature at a field of 100 Oe. The<br />

curves obta<strong>in</strong>ed are displayed <strong>in</strong> Figure 15. The field-cooled magnetization (FC) shows a<br />

rapid <strong>in</strong>crease <strong>in</strong> M below TN= 8 K. The zero-field-cooled magnetization (ZFC) measures<br />

upon cool<strong>in</strong>g to 4.2 <strong>in</strong> zero field and heat<strong>in</strong>g the sample under 1000 Oe is less than that of the<br />

FC below TN (it rema<strong>in</strong>s practically constant) and completely similar above the critical<br />

temperature. F<strong>in</strong>ally, when the sample is cooled with<strong>in</strong> the field and upon further heat<strong>in</strong>g <strong>in</strong><br />

zero field, one can observed (<strong>in</strong>set <strong>in</strong> Figure 15) that the remnant magnetization decrease with<br />

<strong>in</strong>creas<strong>in</strong>g temperature and vanishes above 8 K. All these features are characteristic of a<br />

magnetically ordered state below 8 K [47], with the presence of weak ferromagnetism<br />

<strong>in</strong>tr<strong>in</strong>sic to the sample.<br />

As mentioned before the data above 10 K are no affected by the magnitude of the<br />

external field. Thus, measurements at higher fields (0.1 T) were carried out to study the whole<br />

behavior of the magnetic susceptibility without any appreciable sensitivity losses <strong>in</strong> the<br />

measurements. From a plot of the reciprocal molar magnetic susceptibility vs. temperature<br />

classical Curie-Weiss behavior can be deduced above 20 K (see Figure 16), be<strong>in</strong>g Cm= 4.40<br />

cm 3 K/mol and θ= -13.3 K. From the calculated Curie constant a g value of 2.00 can be<br />

derived, <strong>in</strong> good agreement with that calculated from the ESR spectra and with the topology<br />

of the Fe(III) octahedra <strong>in</strong> the title compound.<br />

Figure 15. Thermal dependence of the magnetization at ZFC (black circles) and FC (open circles) for<br />

the Fe(PO 3) 3 compound. Inset shows the zero-field magnetization curve vs. T for the Fe(PO 3) 3<br />

compound cooled under a magnetic field of 100 Oe.

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