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Nearly full-dense and fine-grained AZO:Y ceramics sintered from the corresponding nanoparticles
Nanoscale Research Lettersvolume 7, Article number: 481 (2012)
Aluminum-doped zinc oxide ceramics with yttria doping (AZO:Y) ranging from 0 to 0.2 wt.% were fabricated by pressureless sintering yttria-modified nanoparticles in air at 1,300°C. Scanning electron microscopy, energy-dispersive X-ray spectroscopy, X-ray diffraction analysis, a physical property measurement system, and a densimeter were employed to characterize the precursor nanoparticles and the sintered AZO ceramics. It was shown that a small amount of yttria doping can remarkably retard the growth of the as-received precursor nanoparticles, further improve the microstructure, refine the grain size, and enhance the density for the sintered ceramic. Increasing the yttria doping to 0.2 wt.%, the AZO:Y nanoparticles synthetized by a coprecipitation process have a nearly sphere-shaped morphology and a mean particle diameter of 15.1 nm. Using the same amount of yttria, a fully dense AZO ceramic (99.98% of theoretical density) with a grain size of 2.2 μm and a bulk resistivity of 4.6 × 10−3 Ω·cm can be achieved. This kind of AZO:Y ceramic has a potential to be used as a high-quality sputtering target to deposit ZnO-based transparent conductive films with better optical and electrical properties.
Transparent conductive oxides (TCO) as transparent electrodes have been widely used in thin-film solar cells and flat panel display devices[1, 2]. The commonly applied TCO materials are In2O3:Sn (ITO), SnO2:F (FTO), and ZnO:Al (AZO)[1, 2]. AZO has attracted much interest as a potential substitute for ITO due to the abundance of its constituent elements in nature, relatively low deposition temperature, and stability in hydrogen plasma[2, 3].
The magnetron-sputtering ceramic target is one of the most widely used methods for AZO film deposition. In the sputtering system, the target plays a major role in achieving high-quality films[4–7]. Generally, the target for sputtering TCO films should have a high density, finer grain size, and better conductance[7–11], which will be helpful for avoiding the formation of nodules to prolong the target lifetime[7, 8], increasing the deposition rate and film uniformity and meeting the requirement of direct current (DC) sputtering. The attempts to enhance the density of the AZO ceramic target become a crucial issue for both researchers and target manufacturers[7, 8, 12–14]. Sun et al. fabricated an ultrahigh-density AZO sintered body (>99.7% theoretical density) after pressureless sintering at 1,400°C by adjusting the mass fraction of polyacrylic acid when slip casting a mixture slurry of commercial ZnO and 2 wt.% Al2O3 powders. Hwang et al. found that the preliminary heat treatment under external pressure increased the density and uniformity after a final sintering. The maximum density value of 2 wt.% Al-doped ZnO sintered at 1,350°C was about 5.52 g/cm3 (approximately 98.9% of the theoretical density). Recently, Zhang et al. used a two-step sintering process to obtain the AZO ceramic with a relative density of more than 99% by sintering the 30-nm sol–gel-synthesized AZO nanoparticles at the second-step sintering temperature of 1,000°C for 12 h. To our best knowledge, the nearly full-dense (namely, exceeding 99.9% of the theoretical density) AZO ceramic has rarely been reported and still kept a challenge as before, especially by a simple and low-cost pressureless sintering at a relatively low temperature.
Few studies have also shown that a small amount of a rare earth element such as yttrium introduced into a ZnO matrix can obviously improve the properties of both ZnO films and the corresponding ceramic sputtering targets[15–18]. For example, Han et al. have utilized an electrochemical deposition method to obtain a 3.7 at% yttrium-doping ZnO film with a resistivity of as low as 6.3 × 10−5 Ω cm after post-deposition annealing in nitrogen at 300°C. GfE Co. (Nuremberg, Germany) has produced a novel aluminum-doped zinc oxide ceramic with yttria doping (AZO:Y) target containing a small amount of Y2O3 besides Al2O3, which can be stably sputtered by pulsed DC sputtering technology due to the higher conductivity[17, 18]. Using this kind of target, Tsai et al. found that the thin AZO:Y film deposited at 300°C had the lowest resistivity of 3.6 × 10−4 Ω cm, the highest mobility of 30.7 cm2 V−1·s−1, and the highest carrier concentration of 5.6 × 1020 cm−3.
However, the above mentioned research results mainly focused on the properties of AZO:Y films; the detailed investigation on the influence of Y doping on the mircrostructure and densification of the AZO ceramic target itself is lacking. In this work, we attempted to fabricate highly dense AZO:Y ceramics by pressureless sintering by a coprecipitation process using Y and Al co-doped ZnO nanoparticles as raw materials, and the microstructure and densification of AZO:Y ceramic were investigated.
Synthesis of AZO:Y nanoparticles
Y-doped AZO (AZO:Y) nanoparticles were synthesized by a coprecipitation process, using an AR grade of zinc nitrate, aluminum nitrate, yttrium nitrate, and ammonium acid carbonate as starting materials (all purchased from Sinopharm Group Co. Ltd., Shanghai, China). A 1 M distilled water solution of Zn(NO3)2·6H2O, Al(NO3)3·9H2O, and Y(NO3)2·6H2O, whose amounts were determined by Al2O3/[ZnO + Al2O3] = 2 wt.% and Y2O3/[ZnO + Al2O3] = 0, 0.1, 0.15, and 0.2 wt.% (the corresponding samples being named AZO:Y0, AZO:Y0.1, AZO:Y0.15, and AZO:Y0.2), respectively, were added to 2 M NH4HCO3 solution drop by drop at a constant temperature of 30°C with stirring to produce a mass white precipitate. After aging for 24 h, the precipitate was filtrated and washed several times, followed by drying for 12 h in an oven at 100°C. Then, the precipitate was calcined at 600°C for 2 h to form AZO:Y nanoparticles.
Sintering of AZO:Y ceramics
The as-received AZO:Y nanoparticles were first granulated by spray drying to form larger sphere aggregations with a diameter of approximately 10 μm and then were pressed by uniaxial pressing (50 MPa, 3 min) in a stainless steel die with a diameter of 8 cm. The green bodies were subsequently pressed by cold isostatic pressing (250 MPa, 5 min) and sintered in air for 8 h at 1,300°C in an electric furnace. In order to clearly observe the microstructure and conveniently measure the conductivity, the sintered specimens were ground and polished with a 1-μm corundum slurry and then thermally etched at 900°C for 20 min.
The phases of the AZO:Y nanoparticles and sintered specimens were identified by X-ray diffraction analysis (XRD, D8 Advance, Bruker AXS GmbH, Karlsruhe, Germany) with CuKα radiation (λ = 1.5406 Å) operated at 40 kV and 40 mA and a scanning step of 0.02°/s. The morphology, microstructure, and composition analyses of the AZO:Y nanoparticles and the sintered bodies were performed using a scanning electron microscopy(SEM)/energy-dispersive X-ray analysis (EDAX) system (S-4800, Hitachi Ltd., Tokyo, Japan). The average particle/grain size of the as-calcined nanoparticle or sintered ceramic specimen was estimated from a minimum of 100 particles/grains obtained from the SEM images by the linear intercept method proposed by Mendelson. The densities of the sintered specimens were determined by Archimedes’s method with a densitometer (MH-600, MatsuHaku Electronic Co., Ltd., Taichung, Taiwan). The bulk resistivities were measured by a physical property measurement system (PPMS; Model-9, Quantum Design Inc., San Diego, CA, USA) at room temperature.
Results and discussion
The SEM images of the unmodified (Figure1a) and different amounts of yttria-modified AZO (Figure1b,c,d) nanoparticles after calcination at 600°C for 2 h as well as the plot (Figure1e) of particle sizes estimated from the SEM images as a function of yttria content are shown. All nanoparticle samples exhibit a nearly spherical morphology, and the average particle sizes are 45.5, 21.6, 19.1, and 15.1 nm for the AZO:Y0, AZO:Y0.1, AZO:Y0.15, and AZO:Y0.2 samples, respectively, which show a trend of size decrease with increasing Y2O3 contents. The result of the SEM images suggests that a small amount of Y2O3 addition can remarkably retard the growth of AZO nanoparticles during calcination. In order to explore the phase of AZO:Y nanoparticles after calcination, a 0.2 wt.% Y2O3-doping nanoparticle sample was used to carry out the XRD analysis, as shown in Figure2. It can be seen that all diffraction peaks are only labeled to the wurtzite ZnO structure (JCPDS card no. 036–1451) without any secondary phase diffraction peaks from Al2O3 and Y2O3 or their compound. According to the energy-dispersive X-ray spectroscopy (EDS) analyses of AZO:Y0.2 nanoparticles shown in Figure3, Al species are found, while the trace of Y species cannot be detected due to its trivial content to the EDS detection. It can be summarized that the role of yttria doping in the calcined AZO nanoparticles is to decrease the particle size.
The AZO:Y ceramic was fabricated by pressureless sintering the calcined AZO:Y nanoparticles at 1,300°C in air. Figure4 shows the XRD patterns of the sintered specimens at 1,300°C. For all sintered specimens, except for the main diffraction peaks corresponding to the hexagonal wurtzite ZnO structure, other small peaks are assigned to the ZnAl2O4 phase. Similarly, the phase related to the yttrium dopant cannot be observed. Because the ionic radius of yttrium (approximately 0.90 Å) is larger than that of zinc (approximately 0.74 Å), yttrium is hardly doped into the ZnO lattice. Almost all yttrium will react with Al2O3 to form an Al2Y4O9 phase, as described in the patent and the literature. In addition, we also use EDS to detect a tiny area with Y aggregation around the grain boundary and further verify that the atom ratio of Y to Al is 2.2, which is close to the stoichiometric ratio of the Al2Y4O9 phase (not shown in this paper). Considering the fact that the solubility of the Al element in ZnO is about 0.9 at% as determined by Zhang and that excess Al2O3 totally reacts with both ZnO and Y2O3 to transform into ZnAl2O4 and Al2Y4O9, respectively, the final composition of the sintered ceramic can be approximatively expressed as 97.4 wt.% ZnO:Al + (2.6 to 2.5) wt.% ZnAl2O4 + (0 to 0.2) wt.% Al2Y4O9 with varied Y2O3 doping . Taking the theoretical density (TD) value of ZnO:Al, ZnAl2O4, and Al2Y4O9 as 5.610 g/cm3, 4.640 g/cm3, and 4.520 g/cm3, the reasonable TDs of the final sintered AZO ceramics can be deduced to be 5.585 g/cm3 for the yttria-undoped ceramic and approximately 5.583 g/cm3 for the yttria-modified ceramics using a weighted average calculation. The measured densities and the TDs as a function of Y2O3 concentrations are plotted in Figure5. Increasing the Y2O3 content, the density of the sintered specimen increased from 5.524 g/cm3 (98.90% of TD) without any Y2O3 doping to the highest one of 5.583 g/cm3 (99.98% of TD) with a Y2O3 content of 0.2 wt.%. So, the small amount of Y2O3 addition can obviously enhance the density to be close to the theoretical density. Furthermore, our research also reveals that the Y2O3 content beyond 0.2 wt.% will severely deteriorate the density of the AZO ceramic (not shown here). A doping content of 0.2 wt.% Y2O3 should be the most optimal one.
In order to understand the effect of Y2O3 modification on the microstructure of the sintered AZO ceramics, SEM was employed to observe the polished sample surface, as shown in Figure6a,b,c,d. For the AZO:Y0 sample, one can observe that the grain is not uniform with an average size of about 5.7 μm, and some small white particles with a size of approximately 0.5 μm uniformly disperse in an inner grain and/or grain boundary. These smaller white particles are deemed to be the secondary-phase ZnAl2O4, as described by Han et al. and also determined by EDS analysis as shown in Figure6e,f, where the abundant Al element in the white particles is much higher than that in the AZO:Y grain. In addition, there are some small cavities and microstructural defects in the sintered body. However, with increasing Y2O3 content (shown in Figure6b,c,d), the grain size decreases to 2.0, 2.4, and 2.2 μm for AZO:Y0.1, AZO:Y0.15, and AZO:Y0.2, respectively, where the grains become more uniform than those in the AZO:Y0 sample. Meanwhile, the small cavities and microstructural defects almost disappear with the increase of the Y2O3 content, implying an increase in density. This result is also in accordance with the measured density shown in Figure5. So, the observation on the microstructure demonstrates that the addition of a small amount of Y2O3 may also play a key role in increasing the density, refining the grain, and improving the microstructure uniformity. The reason for achieving a highly dense AZO ceramic with a fine grain can be ascribed to the following two factors: The first may be due to the use of finer AZO:Y raw nanoparticles, which possess a much higher sintering activity. Due to the smallest particle size, AZO:Y0.2 nanoparticles can be easily sintered to bemore dense at a relatively low temperature. The second may be due to the existence of the secondary-phase particles in the grain boundary. Besides ZnAl2O4 particles, the introduction of Al2Y4O9 into the grain boundary by Y2O3 doping can further refine the grain size by inhibiting the grain growth by pinning or dragging the migration of grain boundaries.
Except for a high density and fine grain, a low resistivity of the AZO ceramic target will meet the requirement of DC sputtering with a high deposition rate. To study the effect of yttria addition on the bulk resistivity of the AZO ceramic, PPMS was used to measure the resistivity; the results are listed in Table1. It can be found that the Y2O3 addition in the AZO matrix does not change the resistivity to a great extent. It just varies from 2.1 × 10−3 Ω·cm without yttria addition to 4.6 × 10−3 Ω·cm for the AZO:Y0.2 sample, which is yet to meet the requirement of DC sputtering. The increase in bulk resistivity can be interpreted by the fact that more AZO grains are refined by yttria doping, resulting in more serious grain boundary scattering.
The main focus of this study was to improve the density and microstructure of the AZO ceramic target by introducing a yttria dopant with a low-cost pressureless sintering process. SEM, EDS, XRD, PPMS, and a densimeter were employed to characterize the precursor nanoparticles and the sintered AZO ceramics. Increasing the yttria doping to 0.2 wt.%, the AZO:Y nanoparticle synthesized by a coprecipitation process has a nearly sphere-shaped morphology and a mean particle diameter of 15.1 nm. With the same amount of yttria, a fully dense AZO ceramic (99.98% of TD) with a grain size of 2.2 μm and a bulk resistivity of 4.6 × 10−3 Ω·cm can be achieved. This kind of AZO:Y ceramic has a potential to be used as a high-quality sputtering target to deposit ZnO-based transparent conductive films with higher optical and electrical properties.
physical property measurement system
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The authors gratefully acknowledge the supports from the National Science Foundation of China (20975107, 60806032), the ‘Hundred Talents Program’ of the Chinese Academy of Sciences, the Zhejiang Natural Science Foundation (Y4100169, Y4110463), and the Ningbo Innovative Research Team Program.
The authors declare that they have no competing interests.
YY conceived the study and participated in its design and coordination. PL, MW, TW, and RT carried out the experiments on the fabrication and characterization of the nanoparticles and corresponding sintered ceramic. WS supervised the result analysis and conducted a paper modification as a corresponding author. All authors read and approved the final manuscript.