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Synthesis of LnCrO3 perovskites and their color properties

Síntese de perovskitas LnCrO3 E suas propriedades de cor

ABSTRACT

The aim of this current study was to prepare LnCrO3 (Ln= La, Pr, Nd) in order to investigate the influence of lanthanides ions on the structural and color properties of the chromites. The powders were synthesized by the microwave-assisted auto-combustion method using urea as a fuel. After calcination at 800 and 1000 °C, characterizations were performed by X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), UV–vis spectroscopy and colorimetric analysis using CIE-Lab system. All the samples are considered single phase and nanocrystalline. There were not significant changes in the colorimetric parameters doped with lanthanides ions. The chromites presented colors with greenish gray tones which became darker in the calcined powders at higher temperatures. No change in the pigment color was observed when incorporated into transparent glaze.

Keywords
Perovskite; microwave assisted synthesis; color properties; chromite

RESUMO

O objetivo deste estudo foi preparar LnCrO3 (Ln = La, Pr, Nd) para investigar a influência de íons lantanídeos nas propriedades estruturais e de cor dos cromitos. Os pós foram sintetizados pelo método de auto-combustão assistida por micro-ondas, usando a uréia como combustível. Após a calcinação a 800 e 1000 ° C, as caracterizações foram realizadas por difração de raios X, microscopia eletrônica de varredura, microscopia eletrônica de transmissão, espectroscopia UV-vis e análise colorimétrica usando o sistema CIE-Lab. Todas as amostras são monofásicas e nanocristalinas. Não houve alterações significativas nos parâmetros colorimétricos dopados com íons lantanídeos. As cromitas apresentaram cores com tons de cinza que se tornaram mais escuros nos pós calcinados a temperaturas mais altas. Nenhuma mudança na cor do pigmento foi observada quando incorporada ao esmalte transparente.

Palavras-chave
Perovskita; síntese assistida por microondas; propriedades de cor,; cromita

1. INTRODUCTION

The perovskite type oxides ABO3 presents a structure with larger cations with ionic radius (alkali metal or lanthanide) and occupy the site A cations with smaller radius (transition metal d) and occupies the site B, as well [11 TANAKA, H., MISONO, M. “Advances in Designing Perovskite Catalysts”. Current Opinion in Solid State and Materials Science, v.5, p.381, 2001.]. The ideal structure has cubic symmetry, but distortions to tetragonal, orthorhombic and rhombohedral may occur, determined by the atomic radius and the crystallization temperature [22 PIMENTEL, P.M., BARBOSA, K.M.B., GOMES, D.K.S., et al., “Optical and structural properties of lanthanum chromite synthesized by microwave assisted self-combustion method”. Materials Science Forum, v.881, p.7-11, 2016.].

Lanthanide chromite with perovskite structure, exhibits high mechanical and chemical stability, high electric conductivity for use in SOFC, oxygen sensors, ionic conductors and catalytic activity for the oxidation reaction [33 HO, W.Y., HSU, C.H., TSAI, M.H., et al. “Interlayer effect on characterization of the La–Cr–O coatings with post sputtering annealing treatment”. Applied Surface Science, v.256, p.2705-2710, 2010.

4 QI, H., LUAN, Y., CHE, S., et al. “Preparation, characterization and electrical properties of Ca and Sr doped LaCrO3”. Inorganic Chemistry Communications, v.66, p.33-35, 2016.

5 KHETRE, S.M., JADHAV, H.V., BAMANE, S.R., “Synthesis and characterization of nanocrystalline LaCrO3 by combustion route”. Rasayan Journal of Chemistry, v.2, p.174-178, 2009.

6 AKASHI, T., MARUYAMA, Y., GOTO, T., “Transport of lanthanum ion and hole in LaCrO3 determined by electrical conductivity measurements”. Solid State Ionics, v.164, p.177-183, 2003.

7 JOSE, J., AMETA, J., PUNJABI, P.B., et al. “Lanthnaum chromite oxide catalyst: synthesis, characterization and photocatalytic activity shown in Azure-B Ameta Bull”. Catalysis Society of India, v.6, p.110-118, 2007.

8 RUBIO, D., SUCIU, C., WAERNHUS, I., et al. “Tape casting of lanthanum chromite for solid oxide fuel cell interconnects”. Journal of Materials Processing Technology, p.250, p. 270-279, 2017.
-99 ATHAWALE, A.A., DESAI, P.A., “Silver doped lanthanum chromites by microwave combustion method”. Ceramics International, v.37, p.3037-3043, 2011.]. However, their optical properties have not yet been studied. These materials due to their high temperature and chemical stability could be used as a ceramic pigment. In addition, the possibility of introducing different chromophores ions into a perovskite structure could produce interesting colors. According to the crystalline field theory, the color in the lanthanide ions and in the transition metals d are due to the transition bands f-f and d-d, respectively. Few studies report the synthesis of ceramic pigments containing these two types of chromophores in the same structure.

A good pigment should be able to present interesting properties, such as high temperature resistance, chemical stability, resistance to chemical attack, high surface area and color homogeneity. In this context, several authors have studied pigments containing lanthanides in their composition [1010 PIMENTEL, P.M., LIMA, S.V.M., COSTA, A.F., et al. “Gelatin synthesis and color properties of (La, Pr, Nd) lanthanide aluminates”. Ceramics International, v.43, p.6592-6596, 2017.

11 HARILAL, M., NAIR, V.M., WARIAR, P.R.S., et al. “Electrical and optical properties of NdAlO3 synthesized by an optimized combustion process”. Materials Characterization, v.90, p.7-12, 2014.

12 OPUCHOVIC, O., KREIZA, G., SENVAITIENE, J., et al. “Sol-gel synthesis, characterization and application of selected sub-microsized lanthanide (Ce, Pr, Nd, Tb) ferrites”. Dyes and Pigments, v.118, p.176-182, 2015.
-1313 OLIVEIRA, R.M.P.B., PIMENTEL, P.M., ARAÚJO, J.H., et al. “Microstructural study of neodmium nickelate doped with strontium synthesized by gelatin method”. Advances in Materials Science and Engineering, v.2013, p.1-5, 2013.].

The method of synthesis causes substantial influence on the properties of the pigments obtained [99 ATHAWALE, A.A., DESAI, P.A., “Silver doped lanthanum chromites by microwave combustion method”. Ceramics International, v.37, p.3037-3043, 2011.]. Several routes of synthesis have been used to obtain lanthanum chromite, such as coprecipitation, sol-gel, and combustion and among others [1414 GUIRE, M.R., DORRIS, S.E., POEPPEL, R.B., et al. “Coprecipitation synthesis of doped lanthanum chromite”. Journal of Materials Research, v.8, p.2327-2334, 1993.

15 SHANKER, J., SURESH, M.B., BABU, D.S., “Synthesis, Characterization and Electrical Properties of NdXO3(X=Cr, Fe) nanoparticles”. Materials Today: Proceedings, v.3, p.2091-2100, 2016.

16 BLIGER, S., BLAB, G., FÖRTHMANN, R., “Sol–gel synthesis of lanthanum chromite poder”. Journal of the European Ceramic Society, v.17, p.1027-1031, 1997.

17 ZHANG, Q.W., LU, J.F., SAITO, F., “Mechanochemical synthesis of LaCrO3 by grinding constituent oxides”. Powder Technology, v.122, p.145-149, 2002.
-1818 JIANG, Y.Z., GAO, J.F., LIU, M.F., et al. “Synthesis of LaCrO3 films using spray pyrolysis technique”. Materials Letter, v.61, p.1908–1911, 2007.]. These alternatives methods have been used replacing the solid state reaction method, which generally uses several processing steps and high temperatures, in addition to synthesizing pigments with heterogeneous properties, resulting in low added value to the pigment.

The aim of this current study was to synthesize lanthanum chromite through the microwave assisted self-combustion method for use as a ceramic pigment, analyzing the influence of the f and d transition ions on color properties, the microstructure and the interaction of the pigment with the transparent glaze.

2. MATERIALS AND METHODS

2.1 Materials

The synthesis of the powders was carried out by the microwave assisted combustion method. mixture of reagents used to obtain the samples [22 PIMENTEL, P.M., BARBOSA, K.M.B., GOMES, D.K.S., et al., “Optical and structural properties of lanthanum chromite synthesized by microwave assisted self-combustion method”. Materials Science Forum, v.881, p.7-11, 2016.]. The materials used were urea (CO(NH2)2 as fuel and the metallic nitrates: (LaNO3)3.6H2O (Cr(NO3)3.9H2O, Pr(NO3)3.6H2O, Nd(NO3)3.6H2O as sources of cations.

2.2 Methods

The amount of each reactant mass was calculated from their respective molecular weight. The ratio of the reactants favors the ratio oxidant / fuel = 5/6, according to the chemical propellant. The mixture consists of the following proportions: one mole of metal nitrate (lanthanum, praseodymium and neodymium) to one mole of chromium nitrate, to five moles of urea. The synthesis reaction starts from the dissolution of urea with deionized water in a beaker with constant stirring at 70 °C. Afterwards the urea was completely dissolved, furthermore, chromium nitrate added was dissolved in deionized water at a temperature of about 80 °C. The solution was kept under stirring for about 30 minutes. After that, the metal nitrate was added (lanthanum, praseodymium, or neodymium) dissolved also in deionized water at a temperature of about 90 °C. The proposed idea was to reduce the amount of water with heating to enter into a microwave oven, with autoignition occurring between 5 and 7 minutes. The resulting powders then were calcined at 800 and 1000 ºC for 4 hours in air to obtain products possessing a phase of the perovskite structure.

2.3 Characterization

Phases analysis of powders calcined at 800 and 1000 °C were performed by X-ray diffraction with a Shimadzu diffractometer XRD-6000 model, operating with CuKα radiation. The diffractograms were obtained with angle of 2θ ranging from 10 to 80 degrees. The diffraction patterns were adjusted and refined through the Rietveld method [1919 RIETVELD, H.M., “A profile refinement method for nuclear and magnetic structures”. Journal of Applied Crystallography, v.2, p.65-71, 1969.] making use of the MAUD software [2020 LUTTEROTTI, L., (2006). MAUD, Version 2.046, http://www.ing.unitn.it/wmaud/.
http://www.ing.unitn.it/wmaud/...
]. The morphologies of the powders were obtained through a scanning electron microscope (SEM) of the brand JEOL, JCM-5700 model. The colorimetric measurements of the CIE-L*a*b* was performed by using the colorimeter Gretag Macbeth color-eye 2180. The reflectance spectra were measured using a UV-Visible spectrophotometer Shimadzu, with accessory reflectance UV-2550 with a wavelength in the region of 200-900 nanometers.

3. RESULTS AND DISCUSSION

Fig. 1 shows the X-ray diffraction (XRD) patterns of LnCrO3 (Ln= La, Pr, Nd) at 800 and 1000 °C, respectively. All compounds of LnCrO3 (Ln= La, Pr, Nd) were synthesized as well-crystallized single-phase powders. The identification of crystalline phases through Rietveld refinement, revealed the single phase powders with orthorhombic perovskite structure according to 2104121 (LaCrO3), 156319 (NdCrO3), 331072 (PrCrO3) ICSD database. The effectiveness of the synthesis method to obtain the perovskite is proven when we compare the results obtained in this work with others reported in the scientific literature [2121 LIU, X., SU, W., LU, Z., “Study on synthesis of Pr1-xCaxCrO3 and their electrical properties”. Materials Chemistry and Physics, v.82, p.327-330, 2003.

22 ALIOTTA, C., LIOTTA, L.F., DEGANELLO, F., et al. “Direct methane oxidation on La1-xSrxCr1-yFeyO3-δ perovskite-type oxides as potential anode for intermediate temperature solid oxide fuel cells. Applied Catalysis B: Environmental, v.180, p.424-433, 2016.

23 SILVA, J.R.R.S., BARROZO, P., MORENO, N.O., et al. “Structural and magnetic properties of LaCrO3 half-doped with Al”. Ceramics International, v.42, p.14499-14504, 2016.
-2424 GUPTA, S., SINGH, P., “Nickel and titanium doubly doped lanthanum strontium chromite for high temperature electrochemical devices”. Journal of Power Sources, v.306, p.801-811, 2016.].

Based on the XRD data, lattice parameters were calculated and presented in Table 1. It was observed that the crystallite size increased as the calcination temperature increased, ranging from 19.72nm to 36.32nm, 15.73nm to 24.08nm and 15.74nm to 17.73 nm to the samples LaCrO3, PrCrO3 and NdCrO3, respectively. This result demonstrates that the average size of the crystallite increases with temperature, which is an expected behavior due to the fact that temperature is the driving force that causes the particles to grow and coalesce [2525 OLIVEIRA, F.S., PIMENTEL, P.M., OLIVEIRA, R.M.P.B., et al. “Effect of lanthanum replacement by strontium in lanthanum nickelate crystals synthetized using gelatin as organic precursor”. Materials Letters, v.64, p.2700-2703, 2010.]. The goodness of fitted (GoF) values of all the fitted patterns lie between 1.58 and 1.86, suggesting a good agreement between the experimental and refined diffraction data [2626 PIMENTEL, P.M., DUTRA, J.L.S., LIMA, A.C., et al. “Structural and magnetic characterization of LaFe1-xAlxO3 (x= 0 and 0.2) orthoferrites synthesized by gelatin method”. Materials Science Forum, v.899, p.227-231, 2017.].

Figure 1
XRD patterns of PrCrO3, NdCrO3 and LaCrO3 a) at 800 °C and b) at 1000 °C.
Table 1
Microstructural parameters of LnCrO3 (Ln= La, Pr, Nd)

SEM images in Figure 2 shows the sample the NdCrO3 at 800 and 1000 °C, respectively. The sample presented a spongy aspect, highly porous structure and a rough surface. The combustion reaction with urea presents a great evolution of gases, results in porous structures with smaller particle size [2727 SILVA, A.L.A., CONCEIÇÃO, L., ROCCO, A.M., et al. “Synthesis of Sr-doped LaMnO3 and LaCrO3 powders by combustion method: structural characterization and thermodynamic evaluation”. Cerâmica, v.58, p.521-528, 2012.]. Spherical particles (< 200 nm) could be seen in HR-TEM images in Figure 3. Nanoparticles result in less flocculation on the glaze surface and better color distribution due to high surface area [2828 DUTRA, J.L.S., DANTAS, G.C.B., PIMENTEL, P.M., et al. “Caracterização óptica e estrutural de ortoferritas de lantânio dopadas com cromo e aluminio”. Cerâmica, v.64, p.1-7, 2018.].

Figure 2
SEM images of the NdCrO3 calcined at (a) 800 °C and b) 1000 °C.
Figure 3
TEM images of the LaCrO3 calcined at 1000 °C.

Reflectance spectra in the UV-Visible region of powders synthesized at temperatures of 800 ° C and 1000 ° C are shown in Figure 4 and 5 for the composition of the perovskites NdCrO3, LaCrO3 and PrCrO3 at temperatures 800 and 1000 °C, respectively. In the synthesized perovskite ions there are two chromophores ions, which are transition elements "d" and the lanthanides (transition "f"), in which the color pigment is a result of transitions d-d and f-f, respectively. The lanthanum does not have f-orbital, but is included in the lanthanide series by having chemical properties similar to other elements in the series, hence in the perovskite LaCrO3, the Cr3+ ion is the only chromophore.

Figure 4
Reflectance spectra of the perovskites NdCrO3, PrCrO3 and LaCrO3 calcined a) at 800 and b)1000 °C.

Comparing the three reflectance spectra and the colorimetric parameters (Table 2), it was observed a difference in the parameters of the three synthesized compounds, which indicates that the contribution of the color is mainly due to the d transition chromophore in the B site of the perovskite. This is proven with the reflectance spectra, since the bands assigned to Cr3+ are wider and more intense in the visible region. This could be clearly seen from compounds of lanthanum and praseodymium, which have quite similar reflectance curves. As the temperature increases, the percentage of reflectance decreases and also decreases the luminescence (lower L value), hence the color becomes slightly darker at higher temperatures. The region between 200 and 370 nm is a region with a low percentage reflectance (high absorption) and does not influence the color, because it occurs outside the visible region (UV); above this, the percentage reflectance starts increasing abruptly. The broad band between 400 and 550 is attributed to the blue region, the intense band near 600 indicates that the material is reflecting in the green region.

In all spectra it was observed spectral bands of the Cr3+ ion in the octahedral site. In the region between 410 and 490 nm the band is well defined and it is attributed to the 4A2g (4F) → 4T1g (4F) transition. The band between 500 and 600 nm is attributed to the 4A2g (4F) → 4T2g (4F) transition. The bands between 660 and 730 nm are less pronounced and they are attributed to 4A2g (4F) → 4T1g (2G) and 4A2g (4F) 2E (2G) transitions [2929 DONDI, M., GRUCIANE, G., GUARANI, G., et al. “The role of counterions (Mo, Nb, Sb, W) in Cr, Mn, Ni - and V doped rutile ceramic pigments Part 2. Colour and technological properties”. Ceramics International, v.32, p.393-405, 2006.].

In the chromite praseodymium spectra (Figure 4) were not observed bands attributed to the transitions of the Pr3+ ion transitions, once they occur in the same region of Cr3+ band. These bands are wider and larger and overlaps the praseodymium bands. In the neodymium chromite spectra (Figure 3), in addition to the chromium ion bands there were also observed some bands of the neodymium ion in the region between 720 and 760 nm, which can be attributed to the 4I9/2 → (4F7/2 + 4S3/2) transitions. The band between 790 and 820 nm is attributed to the 4I9/2 → (4F5/2 + 2H9/2) transition and it is the reason of some neodymium compound be used as lasers [2929 DONDI, M., GRUCIANE, G., GUARANI, G., et al. “The role of counterions (Mo, Nb, Sb, W) in Cr, Mn, Ni - and V doped rutile ceramic pigments Part 2. Colour and technological properties”. Ceramics International, v.32, p.393-405, 2006.].

The coordinates a* and b* are chromaticity coordinates. When the coordinate a* is low and negative it deviates from the green hue. An important observation is that the pigments on ambient light show green color, but the colorimetric coordinates indicated greenish gray tones, this is probably due to some interaction of samples with the excitation lambda of the colorimeter.

Table 2
Colorimetric parameters of LnCrO3 (Ln= La, Pr, Nd) at 800 and 1000 °C

The Table 3 presents the colorimetric parameters of glaze. The chemical composition of transparent glaze consisted of SiO2 (64.57%), Al2O3 (21.25%), CaO (6.61%), K2O (3.43%), ZnO (3.21%) and traces of SO3, Fe2O3, TiO2, CuO oxides. It was observed that the parameters a* and b* of the glazes underwent displacement, however, the color of the pigments were not altered. This was due to the high content of silica and alumina combined with the low content of zirconium oxide and impurities of less than 1% (Table 4), conferring the low reactivity, thermal stability and chemical compatibility between pigment and glaze compounds [3030 AHMADI, S., AGHAEI, A., YEKTA, B.E., “Synthesis of Y(Al,Cr)O3 red pigments by co-precipitation method and their interactions with glazes”. Ceramics International, v.35, p.3485-3488, 2009.]. The brightness values ​​L* of the pigment and the glaze were similar, as compared in Tables 2 and 3. This fact occurred due to the intermediate levels of CaO and K2O that are responsible for the color development. Glazes with high contents of these compounds have lower luminosity and therefore, the final color is darker [3131 PEREIRA, O.C., BERNARDIN, A.M., “Ceramic colorant from untreated iron ore residue”. Journal of Hazardous Materials, v.233-234, p.103-111, 2012.].

Table 3
CIE-L*a* b* coordinates of glazes calcined at 800 °C and 1000 °C

4. CONCLUSION

The microwave assisted combustion method used in this work compared to other methods of synthesis, presented a favorable route for obtaining the LaCrO3, PrCrO3 and NdCrO3 perovskites. The oxides obtained at two temperatures of calcination (800 and 1000 °C) were single phase, nanometric with orthorhombic perovskite structure. The chromite lanthanides showed greenish gray shades when subjected to a colorimeter, being darker in the calcined powders at higher temperatures. It was observed that the transition metal d exerts a greater contribution to the color definition of the lanthanides, since there was a little change in the color with the replacement of the A site in the perovskite. The color of the pigment remained practically unchanged in the transparent glaze, revealing a chemical compatibility between the constituents of the pigments and the glaze.

REFERENCES

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  • 2
    PIMENTEL, P.M., BARBOSA, K.M.B., GOMES, D.K.S., et al, “Optical and structural properties of lanthanum chromite synthesized by microwave assisted self-combustion method”. Materials Science Forum, v.881, p.7-11, 2016.
  • 3
    HO, W.Y., HSU, C.H., TSAI, M.H., et al “Interlayer effect on characterization of the La–Cr–O coatings with post sputtering annealing treatment”. Applied Surface Science, v.256, p.2705-2710, 2010.
  • 4
    QI, H., LUAN, Y., CHE, S., et al “Preparation, characterization and electrical properties of Ca and Sr doped LaCrO3 Inorganic Chemistry Communications, v.66, p.33-35, 2016.
  • 5
    KHETRE, S.M., JADHAV, H.V., BAMANE, S.R., “Synthesis and characterization of nanocrystalline LaCrO3 by combustion route”. Rasayan Journal of Chemistry, v.2, p.174-178, 2009.
  • 6
    AKASHI, T., MARUYAMA, Y., GOTO, T., “Transport of lanthanum ion and hole in LaCrO3 determined by electrical conductivity measurements”. Solid State Ionics, v.164, p.177-183, 2003.
  • 7
    JOSE, J., AMETA, J., PUNJABI, P.B., et al “Lanthnaum chromite oxide catalyst: synthesis, characterization and photocatalytic activity shown in Azure-B Ameta Bull”. Catalysis Society of India, v.6, p.110-118, 2007.
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    RUBIO, D., SUCIU, C., WAERNHUS, I., et al “Tape casting of lanthanum chromite for solid oxide fuel cell interconnects”. Journal of Materials Processing Technology, p.250, p. 270-279, 2017.
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    ATHAWALE, A.A., DESAI, P.A., “Silver doped lanthanum chromites by microwave combustion method”. Ceramics International, v.37, p.3037-3043, 2011.
  • 10
    PIMENTEL, P.M., LIMA, S.V.M., COSTA, A.F., et al “Gelatin synthesis and color properties of (La, Pr, Nd) lanthanide aluminates”. Ceramics International, v.43, p.6592-6596, 2017.
  • 11
    HARILAL, M., NAIR, V.M., WARIAR, P.R.S., et al “Electrical and optical properties of NdAlO3 synthesized by an optimized combustion process”. Materials Characterization, v.90, p.7-12, 2014.
  • 12
    OPUCHOVIC, O., KREIZA, G., SENVAITIENE, J., et al “Sol-gel synthesis, characterization and application of selected sub-microsized lanthanide (Ce, Pr, Nd, Tb) ferrites”. Dyes and Pigments, v.118, p.176-182, 2015.
  • 13
    OLIVEIRA, R.M.P.B., PIMENTEL, P.M., ARAÚJO, J.H., et al “Microstructural study of neodmium nickelate doped with strontium synthesized by gelatin method”. Advances in Materials Science and Engineering, v.2013, p.1-5, 2013.
  • 14
    GUIRE, M.R., DORRIS, S.E., POEPPEL, R.B., et al “Coprecipitation synthesis of doped lanthanum chromite”. Journal of Materials Research, v.8, p.2327-2334, 1993.
  • 15
    SHANKER, J., SURESH, M.B., BABU, D.S., “Synthesis, Characterization and Electrical Properties of NdXO3(X=Cr, Fe) nanoparticles”. Materials Today: Proceedings, v.3, p.2091-2100, 2016.
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    BLIGER, S., BLAB, G., FÖRTHMANN, R., “Sol–gel synthesis of lanthanum chromite poder”. Journal of the European Ceramic Society, v.17, p.1027-1031, 1997.
  • 17
    ZHANG, Q.W., LU, J.F., SAITO, F., “Mechanochemical synthesis of LaCrO3 by grinding constituent oxides”. Powder Technology, v.122, p.145-149, 2002.
  • 18
    JIANG, Y.Z., GAO, J.F., LIU, M.F., et al “Synthesis of LaCrO3 films using spray pyrolysis technique”. Materials Letter, v.61, p.1908–1911, 2007.
  • 19
    RIETVELD, H.M., “A profile refinement method for nuclear and magnetic structures”. Journal of Applied Crystallography, v.2, p.65-71, 1969.
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    LUTTEROTTI, L., (2006). MAUD, Version 2.046, http://www.ing.unitn.it/wmaud/
    » http://www.ing.unitn.it/wmaud/
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    LIU, X., SU, W., LU, Z., “Study on synthesis of Pr1-xCaxCrO3 and their electrical properties”. Materials Chemistry and Physics, v.82, p.327-330, 2003.
  • 22
    ALIOTTA, C., LIOTTA, L.F., DEGANELLO, F., et al “Direct methane oxidation on La1-xSrxCr1-yFeyO3-δ perovskite-type oxides as potential anode for intermediate temperature solid oxide fuel cells. Applied Catalysis B: Environmental, v.180, p.424-433, 2016.
  • 23
    SILVA, J.R.R.S., BARROZO, P., MORENO, N.O., et al “Structural and magnetic properties of LaCrO3 half-doped with Al”. Ceramics International, v.42, p.14499-14504, 2016.
  • 24
    GUPTA, S., SINGH, P., “Nickel and titanium doubly doped lanthanum strontium chromite for high temperature electrochemical devices”. Journal of Power Sources, v.306, p.801-811, 2016.
  • 25
    OLIVEIRA, F.S., PIMENTEL, P.M., OLIVEIRA, R.M.P.B., et al “Effect of lanthanum replacement by strontium in lanthanum nickelate crystals synthetized using gelatin as organic precursor”. Materials Letters, v.64, p.2700-2703, 2010.
  • 26
    PIMENTEL, P.M., DUTRA, J.L.S., LIMA, A.C., et al “Structural and magnetic characterization of LaFe1-xAlxO3 (x= 0 and 0.2) orthoferrites synthesized by gelatin method”. Materials Science Forum, v.899, p.227-231, 2017.
  • 27
    SILVA, A.L.A., CONCEIÇÃO, L., ROCCO, A.M., et al “Synthesis of Sr-doped LaMnO3 and LaCrO3 powders by combustion method: structural characterization and thermodynamic evaluation”. Cerâmica, v.58, p.521-528, 2012.
  • 28
    DUTRA, J.L.S., DANTAS, G.C.B., PIMENTEL, P.M., et al “Caracterização óptica e estrutural de ortoferritas de lantânio dopadas com cromo e aluminio”. Cerâmica, v.64, p.1-7, 2018.
  • 29
    DONDI, M., GRUCIANE, G., GUARANI, G., et al “The role of counterions (Mo, Nb, Sb, W) in Cr, Mn, Ni - and V doped rutile ceramic pigments Part 2. Colour and technological properties”. Ceramics International, v.32, p.393-405, 2006.
  • 30
    AHMADI, S., AGHAEI, A., YEKTA, B.E., “Synthesis of Y(Al,Cr)O3 red pigments by co-precipitation method and their interactions with glazes”. Ceramics International, v.35, p.3485-3488, 2009.
  • 31
    PEREIRA, O.C., BERNARDIN, A.M., “Ceramic colorant from untreated iron ore residue”. Journal of Hazardous Materials, v.233-234, p.103-111, 2012.

Publication Dates

  • Publication in this collection
    28 Nov 2022
  • Date of issue
    2022

History

  • Received
    10 Mar 2020
  • Accepted
    28 Feb 2022
Laboratório de Hidrogênio, Coppe - Universidade Federal do Rio de Janeiro, em cooperação com a Associação Brasileira do Hidrogênio, ABH2 Av. Moniz Aragão, 207, 21941-594, Rio de Janeiro, RJ, Brasil, Tel: +55 (21) 3938-8791 - Rio de Janeiro - RJ - Brazil
E-mail: revmateria@gmail.com