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2012, Journal of Applied Physics
ZrO 2 samples with 11% Nd and La doping and with 7, 9, 11, and 13% Gd doping have been prepared by co-precipitation route followed by sintering at 700 C and 1100 C, for potential application as high conductivity electrolytes in solid oxide fuel cells. The samples have been characterized by x-ray diffraction with laboratory x-ray source of Cu K a radiation and extended x-ray absorption fine structure (EXAFS) spectroscopy measurement at Zr K edge with synchrotron radiation. The XRD spectra have been analyzed to determine the structure of the samples and the EXAFS data have been analyzed to find out relevant local structure parameters of the Zr-O and Zr-Zr shells, viz., bond distances, co-ordinations, and disorder parameters. The effect of change in ionic radius as well as concentration of the dopants on the above parameters has been thoroughly studied. The experimental results, in some cases, have also been corroborated by first principle calculations of the energetics of the systems. V C 2012 American Institute of Physics.
ZrO 2 samples with 11% Nd and La doping and with 7, 9, 11, and 13% Gd doping have been prepared by co-precipitation route followed by sintering at 700 C and 1100 C, for potential application as high conductivity electrolytes in solid oxide fuel cells. The samples have been characterized by x-ray diffraction with laboratory x-ray source of Cu K a radiation and extended x-ray absorption fine structure (EXAFS) spectroscopy measurement at Zr K edge with synchrotron radiation. The XRD spectra have been analyzed to determine the structure of the samples and the EXAFS data have been analyzed to find out relevant local structure parameters of the Zr-O and Zr-Zr shells, viz., bond distances, co-ordinations, and disorder parameters. The effect of change in ionic radius as well as concentration of the dopants on the above parameters has been thoroughly studied. The experimental results, in some cases, have also been corroborated by first principle calculations of the energetics of the systems. V C 2012 American Institute of Physics.
Journal of The European Ceramic Society, 2003
The local structure around Zr, Ce and dopant atoms (Fe and Ni) in the ZrO 2 -CeO 2 system investigated by X-ray absorption spectroscopy (XAS) is reported to better understand the tetragonal phase stabilization process of zirconia. The first coordination shell around Zr atoms is not sensitive to the introduction of dopants or to an increase in the ceria content (from 12 to 20 mol%). Ce ions maintain the eight-fold coordination as in CeO 2 , but with an altered bond distance. The formation of vacancies resulting from reduction of Ce atoms can be discarded, because XANES spectra clearly show that Ce ions are preferentially in a tetravalent state. XANES and EXAFS experiments at the Fe K-edge evidence that the local order around Fe is quite different from that of the Fe 2 O 3 oxide. On the one hand, ab initio EXAFS calculations show that iron atoms form a solid solution with tetragonal ZrO 2 . The EXAFS simulation of the first coordination shell around iron evidences that the substitution of zirconium atoms by iron ones generates oxygen vacancies into the tetragonal network. This is a driven force for the tetragonal phase stabilization process. For Ni doped samples, EXAFS results show that Ni-O mean bond length is similar to the distance found in the oxide material, i.e., NiO compound. Besides this result, no evidence of similar solid solution formation for Ni-doped systems has emerged from the EXAFS analysis . #
Journal of Applied Physics, 2013
Experimental results corresponding to the saturation magnetization and coercive field during the decomposition, upon annealing, of bcc and fcc Fe"Cu& ", obtained by mechanical alloying are reported. The overall behavior points out that the decomposition takes place in two steps: (i) at low temperatures a decrease of the saturation magnetic moment as well as an anomalous thermal dependence of coercive field are observed, however, no phase transformation is detected, and (ii) for further annealing temperatures a new phase appears; the magnetization tends to increase and the coercive field abruptly increases.
Journal of Applied Crystallography, 2008
The crystal structure and the local atomic order of a series of nanocrystalline ZrO 2 -CaO solid solutions with varying CaO content were studied by synchrotron radiation X-ray powder diffraction and extended X-ray absorption fine structure (EXAFS) spectroscopy. These samples were synthesized by a pHcontrolled nitrate-glycine gel-combustion process. For CaO contents up to 8 mol%, the t 0 form of the tetragonal phase (c/a > 1) was identified, whereas for 10 and 12 mol% CaO, the t 00 form (c/a = 1; oxygen anions displaced from their ideal positions in the cubic phase) was detected. Finally, the cubic phase was observed for solid solutions with CaO content of 14 mol% CaO or higher. The t 0 /t 00 and t 00 /cubic compositional boundaries were determined to be at 9 (1) and 13 (1) mol% CaO, respectively. The EXAFS study demonstrated that this transition is related to a tetragonal-to-cubic symmetry change of the first oxygen coordination shell around the Zr atoms.
2014
The influence of low concentrations (1 mol %) of few co-dopants (Y2O3, La2O3, CeO2, Gd2O3, Er2O3, ZnO) on the structure and characteristic of 10 mol % scandia stabilized zirconia was studied. Sintering kinetics and thermal expansion coefficients of synthesized solid eletrolytes were determined. It was found that co-doping increased the conductivity of electrolytes at temperature below 550°C. However, at high temperatures, the introduction of co-dopants decreased the conductivity; moreover, this reduction was more severe the more the ionic radii of Zr4+ and co-dopant differ
Zirconia and ceria possess fl uorite-type structure and conduct electricity by means of oxide ion transport through the lattice. On doping, vacancies created at the oxygen site make way for the neighbouring oxygen atoms to ‘hop’ in the direction of electric fi eld. Among doped zirconia, 8 mol% yttria-stabilized zirconia and 9–11 mol% scandiastabilized zirconia exhibit the highest conductivity. Ceria electrolytes require lower operational temperature (~600–800°C) compared to that of zirconia electrolytes (800–1000°C). With improvement in the processing and fabrication techniques, researchers have developed thinner electrolytes to minimize ohmic polarization and enhance the ionic conductivity enabling operation at lower temperatures (~400–600°C). But such electrolytes are required to be supported on electrodes (anode or cathode) and in later times heterostructured bi-, tri- and multi-layered electrolyte films have been constructed. Since the last decade, development of submicron grain size electrolytes and ultimately two-phase materials with nanodimension grain size has shown improvement in ionic conductivity as well as low-temperature workability. The article reviews the turning points in the technological development of fl uorite-based solid oxide fuel cell electrolytes from single-phase micrometer dimension grain size to recently developed two-phase nanocomposites and nanowires, and the successful achievement of its workability at low temperatures (~450°C).
Solid State Ionics, 2012
Scandia-stabilized zirconia (ScSZ) electrolytes exhibit the highest ionic conductivity among all ZrO 2 -based materials. However, a phase transition occurs around 650°C from cubic to rhombohedral β-phase which is unique for Sc-stabilized zirconia and leads to reduced conductivity. The occurrence of this β-phase can be suppressed by co-doping ScSZ. The aims of this study are to confirm the influence of a small amount of Fe 2 O 3 doping on both the stabilization of the cubic phase and the decrease of the sintering temperature and to investigate the influence of this co-doping on the ionic and electronic conductivity of ScSZ. Therefore (ZrO 2 ) 0.90 -(Sc 2 O 3 ) 0.07 -(Fe 2 O 3 ) 0.03 powder has been prepared by precipitation in aqueous solution and sintered at 1380°C to obtain ceramic. The electrical properties (ionic and electronic conductivities) of this ceramic are compared to the ones of Fe-doped YSZ.
2020
15 at% Mg-doped ZrO2 ceramic material was synthesized by solid-state reaction at 1600 oC. Particle size analysis of raw materials mixture depicts the formation of a narrow particle size distribution (PSD) with a mean particle size of about 56 nm. The structural analysis confirms that the assynthesized Mg-doped ZrO2 product is of pure tetragonal phase (t-ZrO2) with a crystallite size of 55.76 nm. The UV–VIS diffuse reflectance spectrum (DRS) showed a maximum %R at 550 nm and the estimated optical bandgap was about 3.83 eV. The morphology of the sample examined by scanning electron microscopy (SEM) shows interconnected grains in the sintered ceramics. Moreover, EDX analyses confirm the presence of Mg, Zr, and O, with a homogenous distribution throughout the sample.
Solid State Ionics, 2014
Scandia-stabilized zirconia (ScSZ) electrolytes exhibit the highest ionic conductivity among all ZrO 2 -based materials. However, a phase transition occurs around 650°C from cubic to rhombohedral β-phase which is unique for Sc-stabilized zirconia and leads to reduced conductivity. The occurrence of this β-phase can be suppressed by co-doping ScSZ. The aims of this study are to confirm the influence of a small amount of Fe 2 O 3 doping on both the stabilization of the cubic phase and the decrease of the sintering temperature and to investigate the influence of this co-doping on the ionic and electronic conductivity of ScSZ. Therefore (ZrO 2 ) 0.90 -(Sc 2 O 3 ) 0.07 -(Fe 2 O 3 ) 0.03 powder has been prepared by precipitation in aqueous solution and sintered at 1380°C to obtain ceramic. The electrical properties (ionic and electronic conductivities) of this ceramic are compared to the ones of Fe-doped YSZ.
Journal of Alloys and Compounds, 2017
The present work looks at the effect of Nb 2 O 5 co-doping on the structure and conductivity of 11 mol.% Sc 2 O 3 stabilized ZrO 2 solid electrolyte for intermediate temperature solid oxide fuel cells. XPS analysis confirmed that niobium exists in 5+ valence state in the sintered stabilized ZrO 2 samples. SEM study performed on sintered samples revealed that the addition of Nb 2 O 5 not only assists in the densification of Sc 2 O 3-ZrO 2 but also leads to exaggerated grain growth. Both XRD and Raman analysis confirmed that addition of up to 1 mol.% of Nb 2 O 5 suppresses the formation of low-conductivity rhombohedral β-phase and leads to the stabilization of cubic phase. For compositions with > 1 mol.% Nb 2 O 5 , a mixture of tetragonal and monoclinic phases was identified. Impedance spectroscopy showed that the total ionic conductivity increases significantly on co-doping with 1 mol.% Nb 2 O 5. This increase is attributed to the enhanced sinterability and decrease in space-charge potential of Nb 2 O 5 co-doped samples. While > 1 mol.% Nb 2 O 5 compositions have low conductivity due to the formation of low conductivity secondary phases.
Microscopy and Microanalysis, 2013
As the presence of Sc 2 O 3 and CeO 2 is known to largely enhance the ionic conductivity in the temperature range of 600-8008C, compared with the conventional yttria-stabilized ZrO 2 , Sc 2 O 3 &CeO 2stabilized ZrO 2 provide its applicability as electrolytes in solid oxide fuel cells. The current study introduces the methodology to synthesize Sc 2 O 3 &CeO 2-stabilized ZrO 2 powders by using co-precipitation technique or high-temperature hydrothermal reaction, and further describes the structural characterization of the zirconia powders synthesized by the above-mentioned two methods. The co-precipitation technique was found to allow obtaining powders of cubic phase, whereas high-temperature hydrothermal synthesis results in the presence of a monoclinic phase as well. The scanning transmission electron microscope observations also confirm that the size of the synthesized ZrO 2 powders in this study is found to be much smaller than that of commercially available powders.
Physica Status Solidi (a), 1993
EPR and Structural Studies of Doped (Zr02)o.8 (Y20Joe2 BY B. N. MISHRA (a), S. V. SHARMA (b), P. CHAND (b), and N. L. SHUKLA (a) Polycrystalline samples of (Zr02)o,8(Y203)o,2 ceramic oxides doped with vanadium, iron, nickel, and cobalt are synthesized and characterized using X-ray diffraction, scanning electron microscopy, and electron paramagnetic resonance techniques. It is observed from EPR studies that the nickel-doped sample exhibits a rather broad signal comprising a large number of narrow lines. It is noted from the XRD and SEM studies that all the samples consist of mainly two phases, monoclinic and tetragonal.
Journal of Electron Spectroscopy and Related Phenomena, 2007
The X-ray photoabsorption spectra of ZrO 2 films with different phase compositions were measured. The analysis of the results obtained shows that due to the site-sensitivity the X-ray photoabsorption spectroscopy is an attractive method for characterization of the ZrO 2 structure. This allows application of the X-ray spectroscopy in investigation of the crystal structure in the various stages of the thin film growth including the initial stage of the ZrO 2 growth.
Chinese Journal of Chemistry, 2007
Electrical conductivity has been measured at different temperatures for ZrO 2 doped with various molar ratios of CuO. The conductivity increases due to migration of vacancies, created by doping. The conductivity was found to increase with increase in temperature till 220 ℃ and thereafter decrease due to collapse of the fluorite framework. A second rise in conductivity around 500 ℃ was observed due to phase transition of ZrO 2. X-ray powder diffraction, DTA and IR studies were carried out for confirming doping effect and phase transition in ZrO 2. Keywords oxide, doping effect, electrical conductivity, XRD X-ray powder diffraction X-ray studies were recorded using Bragg-Bretano Electrical conductivity
Microscopy and Microanalysis, 2013
As the presence of Sc2O3 and CeO2 is known to largely enhance the ionic conductivity in the temperature range of 600–800°C, compared with the conventional yttria-stabilized ZrO2, Sc2O3&CeO2-stabilized ZrO2 provide its applicability as electrolytes in solid oxide fuel cells. The current study introduces the methodology to synthesize Sc2O3&CeO2-stabilized ZrO2 powders by using co-precipitation technique or high-temperature hydrothermal reaction, and further describes the structural characterization of the zirconia powders synthesized by the above-mentioned two methods. The co-precipitation technique was found to allow obtaining powders of cubic phase, whereas high-temperature hydrothermal synthesis results in the presence of a monoclinic phase as well. The scanning transmission electron microscope observations also confirm that the size of the synthesized ZrO2 powders in this study is found to be much smaller than that of commercially available powders.
Journal of Materials Science, 2014
Ce x Zr 1-x O 2 (x = 0.10, 0.16 and 0.33) nano-11 crystalline powders were obtained by a two-step synthesis 12 technique and sintered by spark plasma sintering (SPS). As 13 consequence of the reduction of Ce 4? to Ce 3? species by 14 carbon in the graphite environment in SPS, phase assem-15 blies including tetragonal, monoclinic and pyrochlore 16 phases were generated in the ceramics during the sintering 17 process. The electrical conductivity was highly dependent 18 on phase assembly and atmosphere (N 2 ,H 2 and O 2). A 19 significant decrease in the activation energy was noticed in 20 the ceramics with high pyrochlore content when measuring 21 the conductivity in H 2 atmosphere, consequence of the 22 strong reduction promoted in these ceramics during the 23 measurement. Equal conduction behavior with similar 24 activation energy was observed in all the ceramics when 25 measuring in O 2 atmosphere. 26 27 Keywords CeO 2-ZrO 2 Á Spark plasma sintering Á 28 Pyrochlore Á Electrical conductivity Introduction CeO 2-ZrO 2-based materials have been widely investigated due to their great potential for different applications, such as gas sensors, solid oxide fuel cells (SOFC) or catalytic materials [1-4]. This system has been shown to be a mixed conductor unlike most stabilized zirconias. Whereas the latter are usually pure ionic conductors, the former can exhibit large electronic contributions at moderate temperatures and oxygen activities [5-8]. The defect structure of CeO 2-ZrO 2 has been described by different authors [5, 7-9] and can be summarized as follows. Due to charge neutrality considerations, a Ce 4? ion substituting a Zr 4? cannot affect any additional creation of oxygen vacancies beyond the inherent defect concentration level. However, the presence of Ce 4? ions on Zr 4? sites affects the point defect equilibria involving oxygen vacancies, as the formation of oxygen vacancies might be favored by the large size difference of the two cations (r i (Zr 4?) = 0.72 Å ; r i (Ce 4?) = 0.87 Å , for sixfold coordination) [5, 6, 9, 10]. The second aspect is that Ce 4? ion is easily reduced to Ce 3? under suitably low oxygen partial pressures (10-11 to 10-19 atm) [11, 12]; therefore, charged oxygen vacancies are produced. These vacancies are coupled to free electrons localized on Ce 3? substitutional defects, giving rise to electronic conductivity through electron hopping between cerium ions [5, 7], which is strongly dependent on the ceria content [5]. The mixed conduction makes this system an interesting material for application as SOFC anode [1], and correlation between electrical and structural properties of the ceriazirconia system has been approached in recent studies [7, 13-16]. Boaro et al. [16] have carried out a complete study of the effects of redox history on structural, chemical and electrical properties of Ce x Zr 1-x O 2 (x = 0.20, 0.50 and
Journal of the European Ceramic Society, 2016
Zirconia-based materials are widely investigated and used as electrolytes in solid-oxide fuel cells, oxygen sensors and electrochemical devices. These materials present polymorphism, which has a critical effect on their technologically important properties. The polymorphism is influenced by, among other factors, aliovalent dopant nature and content, grain size and interfacial energy. In this work, we investigated the crystal structure of ZrO 2-12 mol% CaO and −9 mol% Y 2 O 3 dense ceramics as a function of grain size. We found that the samples undergo a phase transition from the t form of the tetragonal phase to the cubic phase with an increase in grain size. This transition is directly detected by Raman spectroscopy and further evidence is given by a change in the activation energy for bulk ionic conduction. The transition occurs at an average grain size greater than 500 nm for both systems.
Chemical Vapor Deposition, 2012
Dense, crack-free thin films (<5 mm) of the nanostructured scandia-zirconia system (Sc 2 O 3 :ZrO 2 ) stabilized in the cubic-fluorite phase (c-ZrO 2 ) are deposited through conventional low-pressure metal-organic(LP-MO) CVD by using b-diketonate metal complexes as precursors [(Zr(tmhd) and Sc(tmhd) 3 , with -tmhd ¼ 2,2,6,6-tetramethyl-3,5-heptanedionate]. The compositional (energy dispersive X-ray spectroscopy -EDX), structural (X-ray diffraction -XRD) and morphological (field emission gunenvironmental scanning electron microscopy -FEG-ESEM) analyses, confirmed the growth of dense partially and fully stabilized ZrO 2 , a suitable electrolyte for solid oxide fuel cells (SOFC). Results of impedance spectroscopy, which investigates the electrical conductivity of coating, deposited as thin as possible to guarantee the uniform covering of a porous substrate, are reported. Results of thin films of yttria-zirconia system (Y 2 O 3 :ZrO 2 ), deposited with the same method, are also reported for comparison.
Ionics, 2020
Copper-doped SrZrO 3 perovskites prepared via solid-state reaction method are studied for structural, morphological, thermal and electrical properties using various characterisation techniques. The X-ray diffraction and Rietveld refinement confirm the monophasic orthorhombic structure of the undoped and doped samples. The shifting of the XRD peaks with doping is the manifestation of dopant Cu into the Zr site of SrZrO 3 lattice. The thermal expansion curves of doped and undoped samples vary linearly with temperature. The conductivity of the samples increases with copper doping. The activation energy of the samples suggests mixed electronic and ionic (protonic) conduction in the present samples. The conductivity of the doped SrZrO 3 increases up to three orders, i.e. 10 −4 S cm −1 at 600°C. The thermal and electrical properties are in the required SOFC range making Cudoped SrZrO 3 suitable for use as cathode materials.
Journal of Physics: Condensed Matter, 2003
We report the results of an extended x-ray absorption fine structure (EXAFS) study of a sample of ZrO 2 prepared by high-energy ball milling. Xray diffraction showed that the sample contained nanocrystals that were predominantly monoclinic with a particle size of 15 nm. The EXAFS for the sample was strongly attenuated in comparison to that for bulk monoclinic ZrO 2 . This has been interpreted as the ball-milled sample containing a large level of disorder whose possible origins are discussed. In contrast, our previous EXAFS studies of nanocrystalline oxides prepared by sol-gel methods have shown that these samples contain well-ordered crystallites with grain boundaries similar to those in bulk materials. It is concluded that ball-milled samples are very different from oxide nanocrystals produced by other techniques.
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