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Developments in Ceramic Materials Research

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Synthesis, Spectroscopic and Magnetic Studies… 99<br />

ordered phases of some of these compounds, neutron diffraction measurements have been<br />

carried out.<br />

2. SYNTHESIS<br />

The M(PO3)3 metaphoshates were synthesized us<strong>in</strong>g the ceramic method. The start<strong>in</strong>g<br />

reagents were the salt or oxide of the metallic cation <strong>in</strong> its oxidation state of +3. The<br />

phosphorous element was <strong>in</strong>corporated to the composition of the correspond<strong>in</strong>g<br />

metaphosphate <strong>in</strong> the form of (NH4)2H(PO4), with a M:P ratio, depend<strong>in</strong>g on the k<strong>in</strong>d of<br />

metaphosphate prepared.<br />

The synthesis of the M(PO3)3 metaphosphates with M III = V, Cr, Mo and Fe, was carried<br />

out us<strong>in</strong>g the ratio M:P of 1:10. This mixture reaction was heated, under air, <strong>in</strong> an alumn<strong>in</strong>a<br />

crucible at 800 °C, after of a previously heat<strong>in</strong>g <strong>in</strong> the, approximately, 300-400 °C range, <strong>in</strong><br />

order to decompose the (NH4)2H(PO4) reagent. Exceptionally, the Cr2(P6O18) phase was<br />

obta<strong>in</strong>ed us<strong>in</strong>g the same conditions but with a Cr:P ratio of 1:5. All the result<strong>in</strong>g phases<br />

exhibit green color [16-18].<br />

Attempts to prepare the Ti(PO3)3 compound by reduction of TiO2 oxide with an excess of<br />

the (NH4)2H(PO4) were unsucceful. This fact can be attributed to the <strong>in</strong>stability of the Ti(III)<br />

cation <strong>in</strong> air. So, the experimental synthetic method was modified, us<strong>in</strong>g as start<strong>in</strong>g reagents<br />

metallic titanium and an excess of (NH4)2H(PO4). A flux of nitrogen was ma<strong>in</strong>ta<strong>in</strong>ed dur<strong>in</strong>g<br />

the reaction time <strong>in</strong> order to avoid the oxidation to Ti(IV). The result<strong>in</strong>g product shows blue<br />

color [19].<br />

3. PHYSICOCHEMICAL CHARACTERIZATION TECHNIQUES<br />

IR spectra (KBr pellets) were obta<strong>in</strong>ed with a Nicolet FT-IR 740 spectrophotometer.<br />

Diffuse reflectance spectra were registered at room temperature on a Cary 5000<br />

spectrophotometer, <strong>in</strong> the range 8000–50000 cm -1 . Mössbauer spectroscopy measurements<br />

were performed <strong>in</strong> the transmission geometry us<strong>in</strong>g a 57 Co-Rh source <strong>in</strong> the constant<br />

acceleration method. Mössbauer spectra at different temperatures were recordered us<strong>in</strong>g a<br />

bath cryostat. The velocity was calibrated us<strong>in</strong>g α Fe foil. The spectra were fitted us<strong>in</strong>g the<br />

NORMOS program. The isomer shifts are quoted relative to α-Fe at 300 K. A Bruker ESP<br />

300 spectrometer, operat<strong>in</strong>g at X and Q-bands, was used to record the ESR polycrystall<strong>in</strong>e<br />

spectra between 4.2 and 300 K. The temperature was stabilized by an Oxford Instrument (ITC<br />

4) regulator. The magnetic field was measured with a Bruker BNM 200 gaussmeter and the<br />

frequency <strong>in</strong>side the cavity was determ<strong>in</strong>ed us<strong>in</strong>g a Hewlet-Packard 5352B microwave<br />

frequency counter. Magnetic measurements were performed on polycristall<strong>in</strong>e samples<br />

between 1.8 and 300 K, us<strong>in</strong>g a Quantum Design SQUID magnetometer (MPMS-7) with a<br />

magnetic field of 0.1 T, at which the magnetization vs. magnetic field is l<strong>in</strong>ear even at 1.8 K.<br />

About 5 g of the M(PO3)3 (M III = Cr, Mo and Fe) were employed <strong>in</strong> the neutron diffraction<br />

experiments, conta<strong>in</strong>ed <strong>in</strong> a cyl<strong>in</strong>drical vanadium conta<strong>in</strong>er and held <strong>in</strong> a liquid helium<br />

cryostat. The high resolution of D2B was used to obta<strong>in</strong> extensive and accurate structural data<br />

for both phases at room temperature over the angular range 0≤ 2θ ≤160°. For the iron

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