Follow:

Thermoanalytical and X-ray Diffraction Studies on the Phase Transition of the Calcium-Substituted La2Mo2O9 System

https://doi.org/10.3390/ma16020813

“An aqueous sol-gel preparation technique was applied for the synthesis of calcium-substituted lanthanum molybdate with the initial composition of La2–xCaxMo2O9–x/2. The influence of the substitution effect, which plays a crucial role in the formation of final ceramics, was investigated. The thermal behavior tendencies of phase transition at elevated temperatures from the monoclinic crystal phase to cubic as well as reversible transformation were identified and discussed in detail. It was proved that the phase transformation in the obtained mixture significantly depends only on the impurities’ amount, while the partial substitution by calcium atoms above the value of x = 0.05 does not create a homogeneous multicomponent system for La2–xCaxMo2O9–x/2 composition.”

“X-ray diffraction (XRD) patterns were recorded in air at room temperature by employing a powder X-ray diffractometer Rigaku MiniFlex II using CuKα1 radiation. XRD patterns were recorded at the standard rate of 1.5 2θ min–1. The sample was spread on the glass holder to obtain the maximum intensity of the characteristic peaks in the XRD diffractograms. The Rietveld refinements of the obtained XRD patterns were performed using X’Pert HighScore Plus version 2.0a software.”

3.2. X-ray Diffraction

In order to prove the crystalline composition in the obtained La2–xCaxMo2O9–x/2 system, the XRD analysis of the corresponding ceramic was also performed. The XRD patterns of all samples that correspond to the data collected in Table 2 are presented in the Appendix B.
Table 2. Crystal system, mass fraction, crystallite size, lattice parameters, and agreement indices for the La2–xCaxMo2O9–x/2 ceramic.
Initial Composition Crystal Phase Crystal System Mass Fraction/% Crystallite size/nm Unit Cell Weighted R Profile Goodness of Fit
a/pm b/pm c/pm
alpha/o beta/o gamma/o
La2Mo2O9 La2Mo2O9 monoclinic 71.4 104.75 1431.438 2145.289 2855.431 12.99106 1.29603
90.00000 90.42323 90.00000
La2Mo2O9 cubic 28.6 47.03 715.106 715.106 715.106
90.00000 90.00000 90.00000
La1.999Ca0.001Mo2O8.9995 La2Mo2O9 monoclinic 48.9 66.33 1432.093 2145.928 2857.133 10.70047 1.87511
90.00000 90.35913 90.00000
La2Mo2O9 cubic 50.4 45.56 715.357 715.357 715.357
90.00000 90.00000 90.00000
CaMoO4 tetragonal 0.7
La1.99Ca0.01Mo2O8.995 La2Mo2O9 monoclinic 54.1 71.50 1431.437 2145.437 2856.032 10.55389 1.79591
90.00000 90.38470 90.00000
La2Mo2O9 cubic 44.2 46.61 715.103 715.103 715.103
90.00000 90.00000 90.00000
La2Mo3O12 monoclinic 1.2 41.08 1739.278 1186.510 1624.259
90.00000 107.93130 90.00000
CaMoO4 tetragonal 0.5
La1.95Ca0.05Mo2O8.975 La2Mo2O9 monoclinic 59.1 70.52 1431.201 2145.733 2857.156 10.32976 1.76384
90.00000 90.35389 90.00000
La2Mo2O9 cubic 40.3 48.10 715.171 715.171 715.171
90.00000 90.00000 90.00000
CaMoO4 tetragonal 0.6
La1.9Ca0.1Mo2O8.95 La2Mo2O9 monoclinic 44.5 35.83 1432.385 2140.825 2855.251 12.83825 2.41047
90.00000 90.15601 90.00000
La2Mo2O9 cubic 49.3 42.06 714.384 714.384 714.384
90.00000 90.00000 90.00000
CaMoO4 tetragonal 3.8
La2Mo3O12 monoclinic 1.4 43.47 1719.584 1166.525 1614.533
90.00000 108.09910 90.00000
La2MoO6 tetragonal 1.0 42.52 582.792 582.792 3031.347
90.00000 90.00000 90.00000
La1.85Ca0.15Mo2O8.925 La2Mo2O9 monoclinic 76.0 66.77 1430.812 2144.216 2854.451 16.89944 2.2630
90.00000 90.36139 90.00000
La2Mo2O9 cubic 17.1 44.52 714.631 714.631 714.631
90.00000 90.00000 90.00000
CaMoO4 tetragonal 5.8 59.84 526.101 526.101 1153.607
90.00000 90.00000 90.00000
La2Mo3O12 monoclinic 1.1 42.68 1732.883 1168.940 1619.405
90.00000 107.77000 90.00000
La1.8Ca0.2Mo2O8.9 La2Mo2O9 monoclinic 56.2 45.44 1428.985 2143.602 2858.397 12.46852 2.36196
90.00000 90.31453 90.00000
La2Mo2O9 cubic 36.4 46.98 714.584 714.584 714.584
90.00000 90.00000 90.00000
CaMoO4 tetragonal 7.4 58.26 525.675 525.675 1151.621
90.00000 90.00000 90.00000
La1.75Ca0.25Mo2O8.875 La2Mo2O9 monoclinic 79.6 45.63 1430.900 2142.097 2850.290 14.09104 1.54335
90.00000 90.29116 90.00000
La2Mo2O9 cubic 12.2 39.32 714.035 714.035 714.035
90.00000 90.00000 90.00000
CaMoO4 tetragonal 6.4 48.20 523.288 523.288 1146.182
90.00000 90.00000 90.00000
La2Mo3O12 monoclinic 1.8 46.96 1732.404 1167.824 1617.912
90.00000 107.70840 90.00000
La1.7Ca0.3Mo2O8.85 La2Mo2O9 monoclinic 76.1 64.96 1430.166 2143.528 2854.548 13.81435 1.44730
90.00000 90.34066 90.00000
La2Mo2O9 cubic 13.8 45.66 714.447 714.447 714.447
90.00000 90.00000 90.00000
CaMoO4 tetragonal 9.1 67.30 523.476 523.476 1146.807
90.00000 90.00000 90.00000
La2Mo3O12 monoclinic 1.0 66.99 1733.132 1169.219 1619.159
90.00000 107.79630 90.00000
Meanwhile, Figure 5 is consistent with XRD data, which show the formation process and trends of La1–xCaxMo2O9–x/2 and CaMoO4 crystalline phases. As it seen, the enthalpy of the phase transition for La2Mo2O9 mostly depends on the amount of the monoclinic phase in the ceramic mixture. This assumption is confirmed by the increased stabilization of the cubic phase up to 48.0% even after insignificant substitution of lanthanum by calcium ions in the La1.999Ca0.001Mo2O8.9995 system.
Figure 5. XRD patterns of the La1–xCaxMo2O9–x/2 ceramic heat-treated at a 1000 °C temperature.
Nevertheless, by a further increase in the substitution degree of lanthanum by calcium (x = 0.01 and 0.05), the amount of the monoclinic phase for the La2Mo2O9 compound slightly increases; however, the trend of phase transition enthalpy change remains in a decreasing manner as concluded from Figure 3. Considering the fact that the amount of impurity phases in the obtained ceramics is really small, this decrease in the enthalpy of phase transition is basically determined by the increase in the concentration of the mixed-phase La2–xCaxMo2O9–x/2. This statement is partially confirmed by the XRD diffractogram of the Ca1.9Ca0.1Mo2O8.95 compound, in which quite a significant amount of the crystalline side phase for the CaMoO4 was identified. It seems that this impurity phase effect reduces the amount of the La2–xCaxMo2O9–x/2 homogeneous phase in the mixture and creates conditions for the formation of pure La2Mo2O9 compound. This explains the increase in the phase transition enthalpy in La1.9Ca0.1Mo2O8.95 and La1.85Ca0.15Mo2O8.925 samples during both cooling stages (Figure 4). Meanwhile, by the further increase in the calcium substitution degree in the La2–xCaxMo2O9–x/2 system, the decrease in the phase transition enthalpy is already determined by a significant lack of the La2Mo2O9 crystalline phase. This conclusion is confirmed by the constant increase in the concentration of the crystalline phase of calcium molybdate in the final mixture of the obtained ceramics.

Leave a Comment