Effect of the processing parameters on the crystalline structure of lanthanide orthotantalates

Effect of the processing parameters on the crystalline structure of lanthanide orthotantalates

Kisla P. F. Siqueira; Anderson Dias^*

Departamento de Química, Universidade Federal de Ouro Preto-UFOP, Campus Morro do Cruzeiro, ICEB II, Sala 67, CEP 35400-000, Ouro Preto, MG, Brazil

ABSTRACT

The influence of the synthesis parameters on the crystalline structures of orthotantalate ceramics has been investigated. Powder materials were prepared by the solid-state reaction route. X-ray diffraction and Raman scattering measurements were employed to investigate the crystal structure of the produced materials. In this work, we analyzed three different examples in which the temperature and time were decisive on the final crystal structure of LnTaO₄ compounds besides the lanthanide ionic size. Firstly, the thermal evolution for NdTaO₄ samples showed that mixed crystal phases are formed up to 1100 ºC, while well-crystallized M-NdTaO₄ (I2/a) materials are obtained in temperatures higher than 1200 ºC. Also, the influence of the synthesis time was investigated for the LaTaO₄ ceramics: it was necessary 14 h to obtain samples in the P2₁/c structure. Finally, two polymorphs could be obtained for the DyTaO₄ ceramics: P2/a and I2/a space groups were obtained at 1300 ºC and 1500 ºC, respectively. This study indicated that the temperature, time and lanthanide size are directly correlated with the crystalline arrangement of the orthotantalate materials.

Keywords: solid-state processing, lanthanide orthotantalates, crystal structure, Raman spectroscopy

1. Introduction

Ceramic materials have always been, and will continue to be, an inseparable part of human life. They are essential constituents in all modern technologies and devices including computers, displays, solid-state phosphors, photocatalysts, batteries, cars, spacecrafts among others^1,2. Due to their unique combination of properties, such as hardness, high chemical and electrochemical stabilities, photo-electronic activity, ion-conductivity, luminescence and magnetic behavior, ceramic materials have become irreplaceable in a broad variety of applications^3-7. The focus of this work is the lanthanide orthotantalates (LnTaO₄), which belong to the class of electroceramics and have been extensively studied in recent years because of their huge range of environmental- and energy-related applications^8,9.

A series of polymorphic modifications, which belong to the structures usually found in BaMnF₄, M- and M'-fergusonite and scheelite, are known for LnTaO₄ compounds^10-13. The samples with larger ionic radius of Ln (Ln = La-Pr) exhibit two perovskite-like layered polymorphic modifications with monoclinic LaTaO₄-type and BaMnF₄-type structures. The other lanthanides (Ln = Nd-Lu) crystallize in the monoclinic form, besides their ability to possess two fergusonite-type structures. The first one belongs to the space group I2/a, known as M-type structure, while the second one belongs to the space group P2/a, called M'-type structure^10,13,14. Implementation of either of these structure types for LnTaO₄ depends not only on the Ln atomic radius, but also on the synthesis conditions during the different sample preparation procedures. This leads to numerous disagreements in the data about how the structural stability ranges as well as in the regions where the polymorphic modifications occur, including their crystal structure and other properties for LnTaO₄^[11-15].

Lanthanide orthotantalates can be prepared by different techniques. However, all of the existing techniques for the preparation of tantalates have two serious drawbacks: they require high temperatures and considerable time because of the low reactivity of the oxides involved and slow diffusion rates¹⁶. In general, the incompatibility between acid-soluble rare-earth oxides and based-soluble tantalum oxides render aqueous solution preparations more difficult¹. Thereby, the most commonly employed methodology for the production of orthotantalates is the solid-state reaction, which requires repeated milling procedures besides high reaction temperatures. Moreover, due to the intermediate compounds that are involved in the synthesis mechanism, the crystalline homogeneity of powder materials is difficult to achieve.

The synthesis parameters have strong influence on the crystal structure, purity, crystalline degree of order, particle size and morphology of the orthotantalate compounds¹⁷. Since all these aspects determine the properties and performance of these materials, the study of their processing conditions becomes very important. At our knowledge, systematic studies concerning the processing of orthotantalates were not yet reported in the literature. We believe that the lack of studies about the methodology for their production is related with the difficult in synthesizing LnTaO₄ samples. This fact motivated our work, whose the goal is discuss the influence of the synthesis parameters such as temperature, time and lanthanide size on the crystal structure resulting of orthotantalates ceramics processed by solid-state reaction.

2. Experimental Procedure

Orthotantalate ceramics were synthesized by using Ln₂O₃ (RE = La, Nd and Dy; >99.9% Sigma-Aldrich) and Ta₂O₅ (>99.9% Sigma-Aldrich) as starting materials through the solid-state reaction. Stoichiometric amounts were weighed and mixed with a mortar and pestle. The mixed powders were calcined in different rates of time and temperature aiming to obtain crystalline structures. Firstly, the fixed time of 6 h were employed to investigate the structural evolution as a function of temperature. After adjusting this parameter, the syntheses occur under different processing times up to 14 h.

All samples were characterized by X-ray diffraction (XRD) using a Shimadzu D-6000 diffractometer with graphite monochromator and a nickel filter in the range of 10-60º2θ (15 s/step of 0.02º2θ), operating with FeKα radiation (λ = 0.1936 nm), 40 kV and 20 mA. The results were automatically converted to CuKα radiation (λ = 0.1540 nm) for data treatment and manipulation. Raman spectra of the synthesized samples were collected in backscattering configuration by using an Horiba/Jobin-Yvon LABRAM-HR spectrometer with the 632.8 nm line of a helium-neon laser (effective power of 6 mW at the sample's surface) as excitation source. This equipment has diffraction gratings of 600 and 1800 grooves/mm, Peltier-cooled CCD detector and confocal Olympus microscope (100× objective). The experimental resolution was typically 1 cm^-1 for 10 accumulations of 30 s. Appropriate interference filter for rejecting laser plasma lines, edge filter for stray light rejection were used. All resulting spectra were corrected by Bose-Einstein thermal factor¹⁸.

3. Results and Discussion

The thermal evolution study for the NdTaO₄ sample was carried out to investigate the influence of the temperature on its crystallization behavior. Figure 1 presents XRD patterns obtained for samples calcined in air at temperatures ranging from 800 to 1300 ºC, for 6 h. Samples synthesized at temperatures below 1000 ºC exhibited mixed crystal phases, including unreacted oxide precursors, metastable tetragonal (T') structures¹⁹, orthorrombic (O) and monoclinic phases (M), corresponding to Nd₃TaO₇ and NdTaO₄, respectively^14,20. The ceramics processed at 1200 ºC and 1300 ºC exhibited very similar result with a high degree of crystallinity, and they could be indexed with ICDD (International Committee for Diffraction Data) card number #33-0941. Figure 1b shows XRD details in the range of 25-31º2θ, where each peak could be identified in agreement with the ICDD cards and previously published works^14,19,20. We can observe that the diffraction patterns of samples heated at 1200 ºC and 1300 ºC exhibit a single monoclinic phase belonging to the space group I2/a (C⁶_2h, #15) with four units per unit cell. For the sample produced at 1300 ºC, the following lattice parameters could be calculated: a = 5.516 Å; b = 11.246 Å; c = 5.116 Å and β = 95.7º.

According to the literature, NdTaO₄ materials present many polymorphs^10,19. At room temperature, this compound crystallizes in the M- and M'-fergusonite structures¹⁰. At low temperatures, the ceramic crystallizes in a metastable tetragonal (T') structure¹⁹, while under high pressures the monoclinic LaTaO₄-type structure can be obtained¹⁰. Although many attempts have been made by several calcining conditions, the polymorphs could not be obtained for the NdTaO₄ in this work. The unique single phase observed was the monoclinic M-fergusonite. Figure 2 plots the relative amount of monoclinic phase in the region of coexisting phases obtained from the XRD patterns. The ratio of the monoclinic (M) phase to the metastable tetragonal (T') phase is determined from the integral intensities of the monoclinic XRD peaks (-121) and (121) and the tetragonal XRD peak (121) using the following relationship^21,22:

where M(%) is the proportion of the monoclinic phase; I_M is the intensity of the peak from the monoclinic phase and I_T is the intensity of the peak from the metastable tetragonal phase. We can observe that the proportion of the monoclinic phase increases with the increasing of the calcining temperature. The variation of the relative amount of each phase as a function of calcining temperature can be explained by the homogenization of the composition and the enhancement of diffusion²¹.

The inset in Figure 2 presents the Raman spectra of samples processed at 800 and 1300 ºC. In the first spectrum, we can observe broad Raman modes corresponding to a mixture of crystal phases. The spectrum for the calcined sample at 1300 ºC shows the presence of all Raman-active modes in agreement with group-theory calculations, as discussed below. In the arrangement I2/a, Nd and Ta ions occupy the Wyckoff position 4e, while two oxygen occupy the site 8f. Based in these occupation sites, the site-group method of Rousseau et al.²³ was applied to obtain the following Raman-active modes:

The results depicted in Figure 2 show that all these bands could be visualized in the ceramic processed at 1300 ºC, which indicates that the single monoclinic phase was obtained as also detected by XRD. All phonon wavenumbers (cm^-1) and assignments for the NdTaO₄ monoclinic sample could be obtained as follows: 109.6 (A_g), 131.4 (A_g), 172.5 (B_g), 187.0 (A_g), 202.7 (B_g), 214.9 (B_g), 229.4 (A_g), 308.0 (B_g), 322.5 (A_g), 344.3 (B_g), 375.7 (B_g), 412.0 (B_g), 433.8 (B_g), 467.7 (A_g), 634.6 (B_g), 641.9 (A_g), 675.8 (B_g), 813.7 (A_g).

After we determine the ideal temperature to produce single phase NdTaO₄, we applied the same conditions to produce the LaTaO₄, i.e. 1300 ºC and 6 h. However, to obtain the lanthanum single-phase was necessary to use longer processing times. For LaTaO₄ ceramics, longer processing times were tested and the evolution of the crystalline phase was monitored till its stabilization. Figure 3 presents typical XRD patterns for samples processed at 1300ºC, for 6 and 14 h. The materials crystallize in the monoclinic structure with space group P2₁/c (C⁵_2h, #14) and Z=4. The main crystallographic planes indexed by the ICDD card #72-1808 are identified in Figure 3. The lattice parameters for each sample were calculated and are showed in Table 1. We can observe a slight change in the parameters from 6 to 14 h, although the parameter b remains the same. The XRD patterns for these two LaTaO₄ samples are very similar with small differences observed at around 37º2θ, as well as the inversion of the relative intensities of the planes (121) and (-121). However, the results from Raman scattering showed significant changes in the spectra for the samples produced for 6 and 14 h. Figure 4 shows the Raman spectra for these two particular samples. The two spectra were superimposed to the better comparison. The black and red spectra correspond to samples calcined for 6 h and 14 h, respectively. It can be observed that the red spectrum presents more defined modes than the black one. We believe that after 6 h of processing the ceramic presents short-range disorder, which could not be detected by XRD.

Raman bands appear broader for LaTaO₄ samples produced for 6 h in comparison with the modes observed after 14 h, which indicates that it is necessary longer processing times to attain a short-range order. For these samples, 36 Raman-active modes are predicted by group-theory (see Table 1), in agreement with our experimental data depicted in Figure 4 (red spectrum). Comparing the results for LaTaO₄ and NdTaO₄ ceramics, we can assert that the processing time to produce a single-phase sample with high degree of crystallinity is related with the nature of the material, in other words, the processing time is strongly related with lanthanide size. For the NdTaO₄ sample (Nd³⁺ = 0.983 Å), it is necessary 6 h of processing at 1300 ºC, while for LaTaO₄ (La³⁺ = 1.032 Å) it is necessary 14 h at this temperature²⁴.

Now we will discuss the influence of processing parameters on the arrangement acquired by orthotantalates. In this case, the polymorphic transitions in the DyTaO₄ sample from M-fergusonite to M'-fergusonite structures may be observed and it was caused by changing only on temperature of synthesis. The DyTaO₄ sample was firstly synthesized at 1300 ºC for fixed times of 6 h (same conditions employed for NdTaO₄). Under these conditions, DyTaO₄ samples crystallized in M'-fergusonite structure with space group P2/a (C⁴_2h, #13) with 2 units per unit cell. In spite that we have already achieved a crystalline phase, our study was beyond and additional experiments were conducted at higher temperatures in order to observe possible phase transitions. After calcining at 1500 ºC, it was observed a new polymorphic form. The DyTaO₄ sample exhibited the same structure of NdTaO₄, i.e. M-fergusonite structure with space group I2/a (#15).

Figure 5 presents the XRD results for these samples produced at low (1300 ºC) and high (1500 ºC) temperatures, for 6 h. Single-phase, crystalline ceramics were obtained after synthesis without contaminants or secondary phases. In the inset of the Figure 5 we can observe the crystallographic projections and their respective Bravais lattice representations, for a better view of the peculiarities of each polymorphic sample. The main difference between these two arrangements is in the coordination of Ta atom, being four for the M-fergusonite structure and six for M'-fergusonite structure¹⁴. Thus, in the M-type structure the Ta atoms have a tetrahedral coordination, while they exist in a distorted octahedron in M'-type. Furthermore, the average Ta-O distance is longer in the M-type structure, which results in a higher unit cell volume for this arrangement¹⁴. The lattice parameters calculated and unit cell volume are present in the Table 2, for a better comparison between the two polymorphs. We can observe that in the both arrangements the relation among the lattice parameters is the same: b > a > c. However, in the sample obtained at low temperature (P2/a) the parameter b is almost the half than the calculated for the sample produced at high temperature (I2/a).

Figure 6 presents the results obtained from Raman scattering measurements at room temperature for the two polymorphs DyTaO₄. In both samples we can observe all the 18 active modes predicted by group-theory. Table 3 shows phonon wavenumbers and assignments of each Raman-active mode. As already presented previously for the NdTaO₄ sample, the group-theory for I2/a structure (Equation 2) is the same that for P2/a space group. Although the structures for both polymorphs exhibit an equal number of Raman-active modes, they present different spectra. In the Figure 6 the blue spectrum corresponds to the M'-DyTaO₄ ceramic, while the red spectrum corresponds to the M-DyTaO₄ compound. We can observe that the red spectrum is very similar with the obtained for NdTaO₄ (see inset of the Figure 3) because both samples belong to the same space group (I2/a). If we compare the spectra of M- and M'-DyTaO₄, we can observe a change (decreasing and increasing) of relative intensity of the modes through the transition M-fergusonite to M'-fergusonite. This difference could be attributed to the new structural arrangement assumed by the sample when it changes from one structure to another. Furthermore, if we observe the assign of active Raman-modes of these fergusonite-type structures (see Table 2), we can assume that the crystalline arrangement regarding the M-type fergusonites seems to favor the A_g modes, while the arrangement observed in M'-type structures seems to favor the B_g modes.

Table 4 presents a summary of all samples produced in these work by different parameters and the respective results. Through the detailed study concerning the processing of these ceramics, we can determine the more simple way to obtain pure, single-phase La, Nd and Dy orthotantalates. Furthermore, we were able to determine the ideal conditions to obtain the DyTaO₄ in both M- and M'-fergusonite arrangements by solid-state chemistry. All these information are very important and we hope that describing the synthesis methodology and results reported here could help in the development of upcoming works related to orthotantalates. It is important to note that the processing conditions and their influence in the final crystal structures are only the first step to obtain samples with high performance in the respective application. Moreover, we can see that the temperature, time and lanthanide size are directly correlated with the crystalline arrangement for the orthotantalate materials.

4. Conclusions

Lanthanide orthotantalates LnTaO₄ (Ln = La, Nd and Dy) were synthesized by solid-state reaction. The processing conditions to obtain all of these ceramics were reported and discussed in detail in this work for the first time in the literature. Particularly, the effects of temperature, time and lanthanide size on the crystal structures were investigated. For the NdTaO₄ compound, the temperature of 1200/1300 ºC and processing times of 6 h were employed to obtain single-phase ceramics with M-fergusonite structure, space group I2/a (C⁶_2h, #15). At temperatures below 1100 ºC, a mixture of crystal phases were found: unreacted precursors, monoclinic (M), orthorhombic (O), and metastable tetragonal (T') structures. The LaTaO₄ crystallizes in the P2₁/c (C⁵_2h, #14) space group at 1300 ºC, for 14 h. It was also produced the two polymorphs for DyTaO₄ compounds. The crystal phase M'-fergusonite (P2/a, C⁴_2h, #13) was obtained at 1300ºC, while the M-fergusonite (I2/a, C⁶_2h, #15) was produced at 1500 ºC. All crystal structures were determined by XRD and Raman scattering. Finally, we could establish a set of processing parameters (temperature, time and ionic radii) that could be related to the final crystal structure exhibited by the lanthanide orthotantalates.

Acknowledgements

The authors thank the financial support from CNPq, FINEP and FAPEMIG.

Received: June 20, 2013

Revised: October 8, 2013

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Publication Dates

• Publication in this collection
  15 Nov 2013
• Date of issue
  Aug 2014

History

• Accepted
  08 Oct 2013
• Received
  20 June 2013