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Developments in Ceramic Materials Research

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Synthesis, Spectroscopic and Magnetic Studies… 129<br />

The magnetic structure of the Cr2(P6O18) phase is shown <strong>in</strong> Figure 25 where only the<br />

(CrO6) octahedron and magnetic moments are represented for clarity. The model implies<br />

antiferromagnetic arrangements between the magnetic moments stabilis<strong>in</strong>g and overall threedimensional<br />

(3D) antiferromagnetic order. The ref<strong>in</strong>ed moments are aligned <strong>in</strong> the (100)<br />

plane po<strong>in</strong>t<strong>in</strong>g 45.3° from the z axis (seee Figure 25). This value <strong>in</strong>duces the weak<br />

ferromagnetism detected <strong>in</strong> the magnetic measurements at low applied fields.<br />

7.2. M(PO3)3 (M= Mo, Fe) Metaphosphates<br />

The neutron diffraction patterns at 2 K for M(PO3)3 (M= Mo, Fe) were collected <strong>in</strong> the<br />

D2B powder diffractometer and are represented <strong>in</strong> Figure 26. The patterns exhibit extra<br />

magnetic peaks <strong>in</strong>dicat<strong>in</strong>g than both compounds are magnetically ordered at 2 K. The<br />

magnetic reflections for the molybdenum metaphosphate exhibit small <strong>in</strong>tensities due to the<br />

low order<strong>in</strong>g magnetic temperature observed <strong>in</strong> this compound. The thermal evolution of the<br />

neutron diffraction patterns for Fe(PO3)3 was followed <strong>in</strong> the D1B <strong>in</strong>strument from 1.5 to 20<br />

K.<br />

M=Fe<br />

M=Mo<br />

2K<br />

* *<br />

RT<br />

*<br />

* 2K *<br />

RT<br />

Figure 26. Comparison of D2B neutron diagrams of (a) Mo(PO 3) 3 (λ= 1.594 Å) and (b) Fe(PO 3) 3 (λ =<br />

2.41 Å), at room temperature and 2 K. The diagrams are shown as a function of the <strong>in</strong>verse of the d<br />

spac<strong>in</strong>g due to the different wavelengths used <strong>in</strong> the measurements. Magnetic ontribution an also<br />

marked.

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