José Miguel
Calatayud
,
Pablo
Pardo
and
Javier
Alarcón
*
University of Valencia, Department of Inorganic Chemistry, Calle Doctor Moliner 50, 46100-Burjasot, Valencia, Spain. E-mail: javier.alarcon@uv.es
First published on 30th June 2015
In this work we report new results on the preparation, characterization and color properties of the inorganic yellow nano-pigmenting system based on monoclinic V–ZrO2 solid solution nanoparticles. The series of solid solution nanopowders were obtained by a polyol technique where the precipitates, obtained after heating at 180 °C ethylene glycol solutions of vanadyl acetonate and zirconium n-propoxide, were annealed at different temperatures up to 1300 °C for a short duration, in order to improve their crystallinity and control the crystalline form of the final nanoparticles. On annealing at around 450 °C highly crystalline tetragonal V-containing zirconia particles were developed, which transform into the monoclinic form of the V–ZrO2 solid solution after subsequent annealing at 800 °C. Interestingly, the final non-aggregated, well-shaped monoclinic zirconia solid solution particles heated even at as high temperatures as 1000 °C, were sized in the nanometric range displaying well-defined faces and edges. The chromatic coordinates of the prepared nano-pigments after annealing at different temperatures between 800 and 1300 °C indicated yellowness values comparable to conventionally prepared micrometric yellow pigments. The stability of the nano-pigments in aqueous dispersions estimated by zeta potential measurements was good with a low degree of particle aggregation. The used polyol-mediated synthesis can be up-scaled on an industrial level in the preparation of zirconia-based nano-pigmenting systems.
More recently and by using methods of preparation of solids which allow the fast progress of the reaction to the final products, its nature and mechanism of formation was described.9–11 It was then confirmed that this pigment is a solid solution of vanadium in monoclinic zirconia as indicated by the results obtained on the lattice parameter variation with increasing the amount of nominal vanadium in a set of samples prepared by the sol–gel technique.11 Likewise, it was demonstrated that the V cation is mainly in the oxidation state +4 replacing Zr(IV) in the monoclinic zirconia lattice. It can be assumed, therefore, that a reasonable comprehension on the structural features of this ceramic pigment exists already. However, the microstructural control of this ceramic pigmenting system was not entirely achieved by the sol–gel technique method of preparation used due to particles' aggregation and large particle size distribution is formed.
Currently, a technological change is taking place in the ceramic pigment industry, since new decorating methodologies are being incorporated to the ceramic industry. The new methodologies are based on the use of stable dispersions of colloidal ceramic pigment particles, which by the ink-jet technology allows a digital decoration. Thus, from some years ago, the new challenge for the ceramic pigmenting science is to obtain the traditional widely-used or new pigments in the form of nanoparticles, which need to be stable in aqueous and/or other media dispersions. Since the prepared V–ZrO2 ceramic pigmenting system by conventional techniques is still extensively used in the ceramic industry, it seems interesting to outline its preparation by techniques that not only allow to reach high reactivity but also the control of particle size below 100 nm and the narrowing of its particle size distributions. Furthermore, the availability of a new yellow basic color especially when the quadrichromy process is used could allow developing saturated colors over the range of firing temperatures between 800 and 1200 °C.
The polyol technique has been used for the preparation of a large variety of solids at the nanoscale level. One of the key-features of this synthetic procedure is its suitability for the preparation of monodisperse and non-agglomerated particles. In the last decade this technique has been widely used for the preparation of metal particles as well as a large variety of multicomponent oxides, phosphates, sulfides and halogenides.12–17 Moreover, the doping of different host lattices has been also achieved by using the polyol technique.18,19
The aim of the present paper is to report on the preparation, characterization and optical properties of well-shaped, non-aggregated V-doped ZrO2 nanoparticles prepared by using a polyol technique as the method of synthesis. Since a subsequent annealing at different temperatures is required to improve the crystallinity and stabilize the monoclinic zirconia structure of the final V–ZrO2 nanoparticles, their further growth and/or aggregation on annealing must be avoided. The dispersability of the obtained nanoparticles in aqueous media will be also assessed. Finally, the comparison of the structural and spectroscopic results on the polyol-mediated synthesized V-doped ZrO2 nanoparticles with the ones previously reported will allow us to confirm the previously proposed mechanism of formation and other described features of this V-containing ZrO2 nano-pigmenting system.
All samples were tested by DTA/TG, using a TG-STDA thermoanalyzer model Mettler Toledo TGA/SDTA851e/LF/1600 under air atmosphere in platinum crucibles, with a heating rate of 10 °C min−1 in the temperature range between 80 and 1000 °C. The reference sample used was α-Al2O3.
X-ray diffraction analysis (model D-8 Advance, Bruker) were performed using CuKα radiation. The diffractometer had 1 and 3 mm divergence and antiscattering slits respectively, and a 3° 2θ range Lynxeye linear detector. The diffractograms were run with a step size of 0.02° 2θ and a counting time of 0.2 s. Crystalline structures were refined with the Rietveld technique, by using X'Pert Highscore Plus software, on diffractograms acquired from 5 to 120° 2θ with a step size of 0.02° 2θ and an accumulated counting time of 2 s. The refinement was started using the P21/c space group and structure parameters derived by Winterer et al. (ICSD 00-37-1484). The crystallite size of samples annealed at 800 °C for short time was also determined by using the X'Pert Highscore Plus software and LaB6 as standard.
Infrared absorption (IR) spectra (Model 320 Avatar, Nicolet) were obtained in the range 2000–400 cm−1 using the KBr pellet method.
Micro-Raman spectra of annealed samples were obtained by means of an iHR320 Yvon Horiba model and a YAG laser at 532 nm with maximum power of 60 mW. The samples were measured in backscattering geometry at room temperature. A 50× microscope objective was used to focus the excitation laser on the sample and collect the scattered light to the spectrometer. More than 3 different areas were analysed per sample, to obtain representative results. Exposure time, number of acquisitions and laser power varied among 5–30 s, 3–10 and 30–60 mW, respectively. Data acquisition was carried out with the LabSpec software packages from Jobin Yvon.
UV-vis diffuse reflectance (DR) spectra of the specimens (Model V-670, Jasco) were obtained using the diffuse reflectance technique in the range of 200 to 2500 nm. L*a*b* parameters of representative specimens were measured with the same spectrophotometer using a standard lighting C, following the CIE-L*a*b* colorimetric method recommended by the CIE (Commision Internationale de l'Eclairage). In this colour system, L* is the colour lightness (L* = 0 for black and 100 for white), a* is the green (−)/red (+) axis, and b* is blue (−)/yellow (+) axis.
The microstructure of the as-precipitated and thermally treated samples was determined by field emission scanning electron microscopy at 20 kV (Model S-4800, Hitachi Ltd, Tokyo, Japan). The samples were prepared by dropping a dispersion of the powders in water directly onto the holder sample. Before the examination all specimens were coated with gold/palladium in an ion beam coater. Elemental analysis using energy-dispersive X-ray spectroscopy (EDX) of the as-prepared and annealed precipitates was also obtained by the same microscope working at 20 kV.
The morphology of pure and vanadium-containing zirconia particles was also examined using transmission electron microscopy (Model 1010, Jeol Ltd, Tokyo, Japan) at an accelerating voltage of 100 kV. Samples were dispersed in water and drops of the dispersion were transferred to a specimen copper grid carrying a lacey carbon film. Image J software was used for the size measurements performed on the micrographs and the subsequent data analysis, including the generation of size distributions.
Surface characterization and colloidal stability of the different materials were evaluated through the determination of ζ-potential in a pH range between 3 and 11 using a Zetasizer Nano ZS (Malvern Instruments) equipment. Aqueous suspensions (0.1 g L−1) of the materials prepared by sonication (10 minutes, 150 W) were adjusted to the different pH values with NaOH and HCl and measurements were replicated three times.
The most commonly used solvent in the polyol-mediated approach for the preparation of nanometric crystalline solids is EG. On increasing the hydrocarbon chain length, i.e. diethylene glycol (DEG), triethylene glycol (TREG), etc., polyols possess higher viscosity and over reducing power relative to EG. Moreover EG was chosen as solvent in our synthesis since it is also useful to facilitate the stabilization of V4+ in the first stage of reaction. The preliminary study of the most suitable type of precursor as well as the concentration of precursors and the temperature and duration of the reaction is compulsory in order to get particles with well-defined size and shape for each compound. From our preliminary assays, it was concluded that for the 0.1 M VxZr1−xO2 solution, suitable precipitates were obtained for all compositions after keeping 2 hours at 180 °C when EG was used. On the contrary, when using DEG as solvent in the preparation of undoped ZrO2, the obtained translucent dispersion was long time stable and no precipitate could be separated by centrifugation at 8000 rpm for 2 h. This behavior could be attributed to the precipitation of smaller particles on using DEG than EG.
It is to be noted that different effects of polyols on the particle size and dispersability of nanoparticles of distinct nature have been reported in the literature.20,21 Thus, for instance, Cai and Wan reported that in the preparation of magnetite nanoparticles by the polyol technique the morphology of the reaction product is quite different depending on the characteristics of the polyol used: EG, DEG, TREG (triethylene glycol) and TTREG (tetraethylene glycol).20 In this case only TREG yields non-agglomerated magnetite nanoparticles with uniform shape and narrow size distribution. Likewise, Wang et al., reported the preparation of Ag nanocubes with controlled lengths below 30 nm by using DEG as solvent.21 In this case, the alternative use of EG or polyols with longer hydrocarbon chains (TEG or TREG) only led to the formation of twinned particles with irregular shapes.
In order to obtain information on the nature of the processes leading to the obtained yellow and green precipitates after heating the starting mixtures of reagents at 180 °C for 2 h, the series of precipitates were characterized by different techniques. The elemental analysis by EDX was done to confirm that both metals, Zr and V, were present in all doped samples. Fig. 1S† displays the EDX spectra for all the prepared precipitates. A decrease of the Zr:V intensity ratio with the increasing of the nominal amount of vanadium can be inferred. The XRD patterns of the obtained precipitates in the full range of nominal compositions did not show any sharp peak, as can be observed in Fig. 2S.† However, a very broad, weak diffraction peak centered at 2θ value of around 30° can be distinguished in the pattern traces, possibly associated with the presence of a small fraction of nanocrystalline tetragonal and/or cubic zirconia in the precipitates. The formation of metal glycolates by reaction of metal alkoxides and EG has been reported in previous works.22,23 The XRD patterns of different glycolates showed a striking similarity in the emergence of diffraction peaks, especially those located at low angle (∼12°),22,23 not detected in the present study. Presence of zirconium glycolate is then discarded in the final precipitates. The IR spectra of precipitates shown in Fig. 3S† allow us to identify the functional groups on the surface of the precipitates. All the IR spectra were similar and beard a strong resemblance to the corresponding to EG.24 This observation could confirm the role played by the EG, mainly as stabilizer of the precipitate surface avoiding agglomeration.
The aforementioned results seem to indicate that the presence of acac prevented the formation of glycolates and that the Zr(OR)4−x(acac)x, formed in the starting mixture of EG and acac and the VOacac, suffered hydrolysis and condensation on heating in the high-boiling point EG solvent, thus controlling the nucleation and growth of nanoparticles.
The V–ZrO2 precipitates obtained with EG were relatively amorphous; nevertheless the aim of this work is to obtain highly crystalline nanoparticles, because the non-crystalline form directly affects both the energy splitting of the d-orbitals in the case of an absorption process originating from d–d transitions and, most crucial, the stability of the chromophore-containing phase, which decreases dramatically. The only way to stabilize the structural and chromatic characteristics of the V- and Zr-containing precipitates is to anneal those precipitates at different temperatures for short times, whereas avoiding aggregation of the crystalline nanoparticles. To design that annealing process, the compositional changes of the precipitates associated with that heating were followed by TG and DTA. The TG and DTA of the precipitates were similar for the different compositions, therefore only graphs corresponding to the samples V0.05Zr0.95O2 and V0.1Zr0.9O2 are shown in Fig. 4S and 5S,† respectively. TG graphs show rapid change in mass loss of around 45% in three steps for all samples. DTA showed an endothermic peak around 100 °C, associated to the loss of physisorbed water molecules, an exothermic peak at around 300 °C coupled with a strong mass loss that is ascribed to the oxidation of EG, an exothermic peak at around 400 °C attributed to the crystallization of tetragonal VxZr1−xO2 solid solution and finally an exothermic peak at around 600 °C associated with the phase transition from the tetragonal VxZr1−xO2 to the monoclinic VxZr1−xO2 solid solution. From the above results the starting annealing temperature to process the obtained VxZr1−xO2 precipitates was 400 °C.
Fig. 1 XRD patterns of VxZr1−xO2 precipitates annealed at 800 °C for 3 h prepared by using EG as solvent. ★ is tetragonal zirconia and ♦ is monoclinic zirconia. |
On comparing the results in the evolution of samples with compositions VxZr1−xO2 prepared by a conventional sol–gel method using ethanol as solvent with those obtained by the polyol method using EG annealed at similar temperatures, the only detected difference is the stabilization of phases displaying the structure of the monoclinic zirconia at slightly lower temperature, i.e. at around 700 °C, in samples prepared by the conventional sol–gel method.
In order to prove the presence of monoclinic zirconia and while discarding the presence of cubic and/or tetragonal zirconia crystalline forms in the final samples, IR and Raman spectra of annealed samples with increasing nominal vanadium load, in the series annealed at 800 °C for 3 h are displayed in Fig. 2 and 3, respectively. As can be seen in Fig. 2a, the IR spectra of annealed VxZr1−xO2 displayed bands at 419, 502, 575 and 746 cm−1 which can be associated with active modes in monoclinic zirconia phase.25 The additional band also detected at 1015 cm−1, can be attributed to VO stretching vibrations.26 The Raman spectra of these samples showed in Fig. 3, displayed bands at 180, 191, 223, 307, 334, 347, 383, 476, 503, 538, 560, 616 y 640 cm−1, which have been attributed to different Raman active modes in monoclinic zirconia.27–29 Interestingly, four characteristic new bands at 286, 406, 706 and 991 cm−1 appeared in all doped samples. These bands were already reported in the literature for V-doped zirconia samples prepared by sol–gel, were assigned to VO bonds.30
Fig. 3 Raman spectra of VxZr1−xO2 precipitates prepared by using EG as solvent after annealing at 800 °C, ♦ is monoclinic VxZr1−xO2, ● is VO bond. |
From the results of the abovementioned experimental techniques, these V-containing ZrO2 nanoparticles prepared by the polyol technique and annealed at 800 °C for short time periods display unequivocally the structure of monoclinic zirconia.
Sample | x = 0 | x = 0.015 | x = 0.03 | x = 0.05 | x = 0.075 | x = 0.1 |
---|---|---|---|---|---|---|
a (Å) | 5.1478 (1) | 5.1459 (1) | 5.1446 (1) | 5.1442 (1) | 5.1439 (1) | 5.1439 (1) |
b (Å) | 5.2014 (1) | 5.1995 (1) | 5.2059 (1) | 5.2059 (1) | 5.2065 (1) | 5.2064 (1) |
c (Å) | 5.3214 (1) | 5.3227 (1) | 5.3170 (1) | 5.3169 (1) | 5.3159 (1) | 5.3157 (1) |
β (°) | 99.138 (2) | 99.124 (1) | 99.186 (1) | 99.193 (1) | 99.199 (1) | 99.195 (1) |
V (Å3) | 140.676 (5) | 140.613 (5) | 140.577 (5) | 140.558 (5) | 140.541 (5) | 140.532 (5) |
Zr (%) | 1 | 0.973 (5) | 0.953 (7) | 0.939 (5) | 0.927 (5) | 0.895 (8) |
V (%) | 0 | 0.016 (5) | 0.028 (7) | 0.048 (5) | 0.064 (5) | 0.098 (8) |
R exp | 2.75 | 2.78 | 2.73 | 2.76 | 2.80 | 2.77 |
R wp | 4.33 | 4.41 | 5.12 | 5.20 | 5.49 | 5.18 |
GoF | 2.47 | 2.51 | 3.51 | 3.54 | 3.85 | 3.51 |
Fig. 5 UV-vis diffuse reflectance spectra of precipitates VxZr1−xO2, 0 ≤ x ≤ 0.1, prepared by using EG as solvent after annealing at 800 °C for 3 h. Inset samples annealed at 1300 °C. |
The evolution with vanadium content of the L*a*b* parameters of samples annealed at 800 °C for 3 h in the series of samples, is shown in Table 2. Also, for the sake of comparison the colorimetric parameters of a conventional vanadium–zirconia pigmenting system are shown in Table 3.32,33 In all V-doped zirconia, those parameters correspond to a yellowish colour, the intensity of which increased on raising the vanadium content up to the specimen with nominal composition V0.075Zr0.925O2. For larger vanadium contents than x = 0.075, the b* parameter decayed. An opposite trend was observed for the parameter a*, whose minimum value was obtained for specimen with x = 0.03.
Fig. 6 TEM micrograph of monoclinic V0.015Zr0.985O2 nanoparticles prepared using EG as solvent and after annealing the precipitate at 800 °C for 3 h. |
Fig. 7 TEM micrograph of monoclinic V0.05Zr0.95O2 nanoparticles prepared using EG as solvent and after annealing the precipitate at 800 °C for 3 h. |
Fig. 8 TEM micrograph of monoclinic V0.1Zr0.9O2 nanoparticles prepared using EG as solvent and after annealing the precipitate at 800 °C for 3 h. |
x = 0 | x = 0.015 | x = 0.03 | x = 0.05 | x = 0.075 | x = 0.1 | |
---|---|---|---|---|---|---|
XRD patterns (nm) | 29 (1) | 37 (1) | 65 (1) | 64 (1) | 65 (1) | 66 (1) |
TEM images (nm) | 43 (2) | 54 (2) | 80 (2) | 82 (1) | 80 (5) | 81 (1) |
Fig. 9 SEM micrograph of monoclinic V0.015Zr0.985O2 nanoparticles prepared using EG as solvent and after annealing the precipitate at 800 °C for 3 h. |
Fig. 10 SEM micrograph of monoclinic V0.05Zr0.95O2 nanoparticles prepared using EG as solvent and after annealing the precipitate at 800 °C for 3 h. |
Fig. 11 SEM micrograph of monoclinic V0.1Zr0.9O2 nanoparticles prepared using EG as solvent and after annealing the precipitate at 800 °C for 3 h. |
An interesting parameter of nanoparticles determined from the broadening of the Bragg peaks in the XRD pattern is the crystallite size. We have determined crystallite sizes of monoclinic VxZr1−xO2 solid solutions previously annealed at 800 °C by the Rietveld method. The corresponding values, in the range over 30 and 70 nm, are included in Table 4. As it can be observed the trend in the series was the same as the observed in the mean diameters of nanoparticles measured on TEM images. The crystallite size increased on doping up to x = 0.03 and from that composition point on, remained constant. Nevertheless, in general, crystallite sizes were a bit smaller than nanoparticle sizes. That small difference between the crystallite site determined from XRD and the averaged particle diameter from TEM images is quite usual and could be due to the overestimation of sizes by measuring particle sizes in images.
Fig. 12 ζ-potential variation of monoclinic ZrO2 and V0.05Zr0.95O2 nanoparticles in aqueous solution. |
Fig. 13 Schematic graph summarizing the low-temperature polyol-mediated process leading to V–ZrO2 nano-pigments. |
The chromatic coordinates of the prepared nano-pigments after annealing at different temperatures between 800 and 1300 °C indicated yellowness values comparable to conventionally prepared micrometric yellow pigments. The stability of the nano-pigments in aqueous dispersions estimated by zeta potential measurements was good and a small degree of particles aggregation occurred.
The use of the polyol-mediated synthesis allowed the preparation of V-containing ZrO2 inorganic yellow nano-pigments by an easy procedure without requiring neither multisequential steps nor advanced experimental conditions or equipment. These characteristics allow using the polyol approach as a suitable way of industrial manufacture of nano-pigments.
From the results obtained in this specific pigmenting ceramic system it can be inferred that the polyol approach can be applied for the preparation of other widely used micrometric ceramic pigmenting systems in the nanometric scale with a good control of the three main characteristics of particles, i.e., size, degree of agglomeration and phase composition.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra08762g |
This journal is © The Royal Society of Chemistry 2015 |