Original Research ARTICLE
Effect of sintering temperature on microstructure, chemical stability, and electrical properties of transition metal or Yb-doped BaZr0.1Ce0.7Y0.1M0.1O3−δ (M = Fe, Ni, Co, and Yb)
- Department of Chemistry, University of Calgary, Calgary, AB, Canada
Perovskite-type BaZr0.1Ce0.7Y0.1M0.1O3−δ (M = Fe, Ni, Co, and Yb) (BZCY-M) oxides were synthesized using the conventional solid-state reaction method at 1350–1550°C in air in order to investigate the effect of dopants on sintering, crystal structure, chemical stability under CO2 and H2S, and electrical transport properties. The formation of the single-phase perovskite-type structure with an orthorhombic space group Imam was confirmed by Rietveld refinement using powder X-ray diffraction for the Fe, Co, Ni, and Yb-doped samples. The BZCY-Co and BZCY-Ni oxides show a total electrical conductivity of 0.01 and 8 × 10−3 S cm−1 at 600°C in wet H2 with an activation energy of 0.36 and 0.41 eV, respectively. Scanning electron microscope and energy-dispersive X-ray analysis revealed Ba and Co-rich secondary phase at the grain-boundaries, which may explain the enhancement in the total conductivity of the BZCY-Co. However, ex-solution of Ni at higher sintering temperatures, especially at 1550°C, decreases the total conductivity of the BZCY-Ni material. The Co and Ni dopants act as a sintering aid and form dense pellets at a lower sintering temperature of 1250°C. The Fe, Co, and Ni-doped BZCY-M samples synthesized at 1350°C show stability in 30 ppm H2S/H2 at 800°C, and increasing the firing temperature to 1550°C, enhanced the chemical stability in CO2/N2 (1:2) at 25–900°C. The BZCY-Co and BZCY-Ni compounds with high conductivity in wet H2 could be considered as possible anodes for intermediate temperature solid oxide fuel cells.
Research on perovskite-type (ABO3) acceptor-doped BaCeO3 materials has been accelerated in recent years due to their attractive high protonic conductivity under H-containing atmospheres (Schober, 2003; Tao and Irvine, 2006; Zuo et al., 2006b; Yang et al., 2009, 2010). Acceptor doping of the perovskite creates oxide ion vacancies in the perovskite structure. Incorporation of H2O into these sites will create mobile proton charge carriers (H+) (Iwahara et al., 1981). These physical properties make them attractive membranes for proton conducting solid oxide fuel cells (H-SOFCs), H2 pumps, gas separation, and steam electrolyzers (Schober, 2003). Despite the high protonic conduction in wet reducing atmospheres, BaCeO3 suffers from chemical instability in CO2 atmospheres, due to BaCO3 formation (Zuo et al., 2006b; Tu et al., 2009). The reaction may proceed to the complete decomposition of BaCeO3 into CeO2 and BaCO3 under CO2 at elevated temperatures (Trobec and Thangadurai, 2008). While hydrocarbons are the ultimate fuels for SOFCs and for H2 production, CO2 exposure is inevitable for anode and electrolyte materials in H-SOFCs. It has been shown that partial Zr-substitution of the Ce-site enhances the chemical stability in CO2 (Ryu and Haile, 1999), with the Zr-dopant significantly suppressing the proton conductivity (Pergolesi et al., 2010). The Zr-doped BaCeO3 was found to decompose in CO2 at 900°C (Zhong, 2007), while it was reported to partially decompose under 20% CO2 at the same temperature (Zuo et al., 2006a).
To overcome the lower ionic conductivity, acceptor dopants have been introduced to the B-site in order to increase the and subsequent proton concentration upon H2O incorporation into the oxide ion vacancies through reaction (1) (Iwahara et al., 1981; Knight, 1999; Kreuer, 1999; Shimura et al., 2005; Azimova and McIntosh, 2009; Ricote and Bonanos, 2010; Zhao et al., 2010),
where and represent oxygen ions in the lattice position and proton attached to lattice oxygen site, respectively. BaZr0.1Ce0.7Y0.2O3−δ (BZCY) is a frontier compound that has out-performed conventional electrolytes at 300–550°C (Zuo et al., 2006b). BaZr0.1Ce0.7Y0.1Yb0.1O3−δ (BZCY-Yb) showed a proton conductivity more than two times that of the BZCY parent compound (Yang et al., 2009). This has initiated several studies aimed at investigating the properties of BZCY-Yb under SOFC anode conditions and attempting to further enhance its catalytic performance (Yang et al., 2010; Liu et al., 2011; Zhang et al., 2012; Nguyen and Yoon, 2013). SOFCs utilizing Ni/BZCY-Yb composites as the anode material have produced a power density of 1.1 W cm−2 at 750°C. Here, we show the results of incorporating a new series of dopants into the B-site of BZCY, resulting in the enhancement of both the electrical conductivity and material sinterability. BZCY-Co, prepared at 1550°C, shows the highest total electrical conductivity of 0.01 S cm−1 at 600°C in wet H2.
Materials and Methods
Perovskites having the nominal chemical formula BaZr0.1Ce0.7Y0.1 M0.1O3−δ (BZCY-M) (M = Fe, Ni, Co, and Yb) were synthesized by the conventional solid-state method in air. Stoichiometric amounts of BaCO3, ZrO2, CeO2, Y2O3, Fe2O3, NiO, Co(NO3)2⋅6H2O, and Yb2O3 were ball milled with zirconia balls for 6 h at 200 rpm in isopropanol. The dried powder mixtures were then calcined at 1100°C for 24 h in air. After cooling and ball-milling for 6 h, powder X-ray diffraction (PXRD) analysis [Bruker D8 powder X-ray diffractometer (Cu Kα, 40 kV; 40 mA)] at room temperature with a 2θ step scan width of 0.02 and a counting time of 6 s was carried out on each sample. The calcination and subsequent ball-milling process was repeated two more times at 1100°C for 12 and 24 h, before a final heat treatment at 1350°C for 6 h. The PXRD data were then used for the analysis of the crystal structures of the Fe, Co, and Ni-doped samples. For comparison, the parent compound (BZCY-Yb) was also synthesized using a similar synthesis method and studied by PXRD. Rietveld refinements were performed using the program GSAS (Larson and Von Dreele, 1994) and EXPGUI interface (Toby, 2001).
For conductivity measurements, the ball milled powders were uniaxially pressed using a 13 mm die at 120 MPa. The pressed samples were sintered at 1250, 1350, and 1550°C for 12 h. Pt paste (LP A88-11S, Heraeus Inc., Germany) was painted on the two sides of the cylindrical samples to serve as the electrodes. The conductivity of the samples was measured using a two-electrode four-probe conductivity measurement setup using the impedance spectroscopy technique, employing either a Solartron 1287/1255 potentiostat/galvanostat/impedance analyzer or a Solartron 1260 impedance analyzer in air and humid H2 (3 vol.% H2O).
The in situ CO2 stability test was performed on powdered samples (weight: 10–20 mg; particle size: <150 μm) using a Mettler Toledo thermogravimetric analyzer (TGA) in CO2/N2 (1:2 ratio). The samples powders were passed through a sieve with mesh number 100 (Endecotts Ltd.) to remove any particle larger than 150 μm. The chemical stability of the materials in the H2S-containing atmosphere was studied at 800°C for 24 h (10°C/min) in 30 ppm H2S in dry H2. The morphology and composition of the samples were determined using a Philips XL 30 scanning electron microscope (SEM) with energy-dispersive X-ray analysis (EDX) capabilities, and also a Zeiss Sigma VP field-emission SEM equipped with an Oxford INCA X-Act EDX unit. The distribution of elements in the samples was also established using wavelength dispersive spectrometry (WDS), employing a JEOL JXA-8200 electron microprobe.
Table 1 shows the Rietveld refinement results for BaZr0.1Ce0.7Y0.1 M0.1O3−δ (M = Fe, Co, Ni, and Yb). The refinement XRD profiles are shown in Figure 1, with the formation of the orthorhombic space group Imam, thus confirmed. The crystal structure involves Ce, Zr, Y, and M sharing the same lattice position. These cations are coordinated by six oxygen ions that form an octahedral geometry, as shown in Figure 2A. Each oxygen anion is bonded to two cations on both sides, leading to corner-sharing between the octahedra (Figure 2A). There are spaces between these octahedra where the large Ba2+ cations reside (Figures 2A,B). The Ce(ZrYM)O6 octahedron is tilted in a direction opposite to all of its nearest neighbors. Therefore, if an octahedron is tilted to the right, all of the nearest neighbor octahedra will be tilted to the left. The Ba atoms have 12 oxygen anions as their nearest neighbors (Figure 2C).
Figure 1. Rietveld refinement profiles for BaZr0.1Ce0.7Y0.1M0.1O3−δ phases synthesized at 1350°C for (A) M = Fe, (B) M = Co, (C) M = Ni, and (D) M = Yb. The arrows in (D) represent the positions where the 201 and 221 peaks would be observed if the space group was Pnma (space group No. 62).
Figure 2. (A) Crystal structure of BZCY-M. The corners of the octahedra are where oxygen ions are located, while the large green spheres represent the Ba atoms. (B) The crystal structure viewed through the a-axis, with the blue spheres showing the Ce/Zr/Y/M atoms, green spheres representing Ba, and red spheres oxygen. (C) The crystal structure viewed through the c-axis, where the Ba atoms are connected to their nearest oxygen atoms. Each oxygen is located between four Ba atoms.
The unit cell volumes for the M = Fe and Co phases are similar to each other (Figure 1), while there is a pronounced increase for the Ni-containing oxide and also a further increase for the Yb-doped material. These observations are consistent with the large ionic radii of Ni2+ and Yb3+ (Shannon, 1976) and support the hypothesis of the substitution of the transition metal dopants in the B(Ce)-site in BZCY. However, the unit cell volume for all four phases is markedly smaller than that of the un-doped BaCeO3, which is 339.86 Å3 (Knight and Bonanos, 1995), due to the effect of the small Zr4+ ion in the doped phases.
Typical AC impedance plots obtained at 484 and 837°C for BaZr0.1Ce0.7Y0.1Ni0.1O3−δ in H2 (+3 vol.% H2O) are shown in Figure 3. The total resistance (bulk + grain boundary + electrode) is used to calculate the conductivity of the investigated samples. At lower temperatures (Figure 3A), three distinct arcs are observed. At higher temperatures, although it seems that the two higher frequency arcs have merged into one arc, the impedance data can still be fitted better by using three RC units, as is shown in the inset of Figure 3B. The magnitude of the constant phase elements (CPE) is larger than values normally attributed to oxygen ion conductors and is close to the capacitance reported for the proton conductors (Petit and Tao, 2013). The conductivity (σ) of the compounds was computed using Eq. 2:
where l, R, and A are the thickness (cm), total resistance (Ω), and cross sectional area (cm2) of the cylindrical sample. Figure 4 shows the Arrhenius plots for the total conductivity of the compounds in air and H2 + 3 vol.% H2O after sintering at 1250, 1350, and 1550°C. Among the 1250 (Figures 4A,D) and 1350°C (Figures 4B,E) sintered samples, the Ni-doped samples show a higher conductivity. However, by increasing the sintering temperature to 1550°C, the Co-doped sample showed the highest conductivity (0.01 S cm−1 at 600°C in wet H2) (Figures 4C,F) of the new compounds synthesized in this study. The conductivity of the Co-doped sample in both air and wet H2 was found to increase by about 10 times by increasing sintering temperature by 300°C, while the conductivity of the Ni-doped sample is suppressed by ca. 3 times. The Fe-doped sample does not show significant changes in conductivity, even after firing at 1550°C, while the BZCY-Co compound, sintered at 1550°C, shows the highest total conductivity of 2.6 × 10−2 S cm−1 at 800°C in air.
Figure 3. Typical AC impedance spectra and fitted lines of the BaZr0.1Ce0.7Y0.1Ni0.1O3−δ compound at (A) 484°C and (B) 837°C in H2 + 3 vol.% H2O. The equivalent circuit and fitted data are shown in the inset.
Figure 4. Arrhenius plots for the total conductivity of the BZCY-M compounds in air (A–C) and H2 (with 3 vol.% H2O) (D–F) after sintering at 1250°C/24 h (A,D), 1350°C/24 h (B,E), and 1550°C/12 h (C,F).
Phase Stability and Sinterability
The sinterability and phase stability of the as-synthesized compounds at three temperatures (1250, 1350, and 1550°C) were also studied. To serve as a proton conductor electrolyte, materials such as BZCY-Yb and BZCY have generally been sintered at high temperatures, e.g., 1550°C, to achieve the minimum porosity (Yang et al., 2009). Co-sintering of the anode and electrolyte, especially in anode-supported SOFCs, is a common cell fabrication method. During the co-sintering of these two materials, the anode materials are exposed to a temperature high enough to achieve electrolyte sintering, and thus their stability at these temperatures is necessary. Therefore, the effect of sintering at 1550°C on the chemical stability and microstructure of the synthesized compounds was investigated. As a reference, the sintering behavior of these compounds is compared with that of BZCY-Yb.
Figures 5A–C show the effect of the sintering temperature on the microstructure of the BZCY-Fe compound. While the sintering process has already started at 1250°C, the dense sample is obtained at 1550°C. The morphology of the BZCY-Ni and BZCY-Co compounds after sintering at different temperatures is shown in Figures 5D–I, respectively. Both samples show a dense morphology even at 1250°C, confirming the effect of Ni and Co as effective sintering aids. By increasing the sintering temperature, the grain size increases considerably. On the other hand, the sintering of the BZCY-Yb compound only begins at 1550°C, and after 12 h of sintering at this temperature; the sample still has some porosity (Figure 5L). Comparing Figures 5J,K, it can be seen that the 1350°C sintering temperature has caused some grain growth, but without noticeable sintering of the BZCY-Yb sample. Also, considering Figures 5H,I, a secondary phase (marked with the letter “S”) is observable in the BZCY-Co sample. Observation of a BaCoO3 phase in a similar system has been reported in the literature (Yang et al., 2011). Based on the SEM image, the secondary phase seems to wet the BZCY-Co grains very well, running into the grain-boundaries. Similar to the BZCY-Co sample, the Ni-doped compound also shows a secondary phase (Figure 5F) after firing at 1550°C in air. However, no secondary phase is observed for the Fe- and Yb-doped samples, even after firing at 1550°C.
Figure 5. Top-view SEM images of the BZCY-M pellet samples, with M = Fe (A–C), Ni (D–F), Co (G–I), and Yb (J–L) after firing at 1250°C/24 h (A,D,G,J), 1350°C/24 h (B,E,H,K), and 1550°C/12 h (C,F,I,L) in air. The secondary phase in the BZCY-Co sample is marked with the letter “S” in (H,I).
The chemical stability of the Ni-, Co-, and Fe-doped BZCY-M compounds was studied in CO2/N2 (1:2 ratio) and in 30 ppm H2S/H2 and results are shown in Figures 6 and 7, respectively. To eliminate the effect of the synthesis method on the stability, the BZCY compound was also synthesized using a similar method (at 1350°C). The BZCY compound shows a minimal conversion to BaCO3, while the 1350°C synthesized doped BZCY-M compounds start to gain weight in the temperature range of 450–500°C (Figure 6A). The decomposition process accelerates at around 600°C and, at 800°C, reaches maximum values of 6, 12, 14, and 17% conversion to BaCO3 for the BZCY-Fe, -Ni, -Co, and -Yb-doped samples, respectively. Interestingly, except for the BZCY sample, the CO2 stability trend of the BZCY-M compounds follows the reverse pattern of the conductivity trend. While the BZCY-Yb and BZCY-Co samples show some of the highest conductivity values among the compounds examined here, they show the highest CO2 uptake and thus the lowest chemical stability. Similarly, the BZCY-Fe compound, with the lowest conductivity, illustrates a lower CO2 uptake and better stability. On the other hand, after the samples were fired at 1550°C for 12 h, the chemical stability in CO2 has increased significantly, with the BZCY-Ni sample not gaining any measurable weight. The percent conversion of the Fe- and Co-doped samples to BaCO3 is also now less than 2%, while the Yb-doped sample still exhibits greater decomposition, with a close to 6% conversion to BaCO3.
Figure 6. Thermogravimetric analysis (TGA) in CO2/N2 (1:2 ratio) at a 10°C/min heating and cooling rate for BaZr0.1Ce0.7Y0.1M0.1O3−δ compounds (M = Fe, Ni, Co, Y, and Yb), synthesized at 1350°C (A) and after firing at 1550°C (B). In order to be able to compare the results, the particle size was controlled at below 150 μm in both cases.
Figure 7. XRD patterns of the BZCY, BZCY-Fe, -Co, and -Ni samples after testing for 24 h at 800°C in dry H2/30 ppm H2S. Small un-identified impurity phase peaks (♦) are observable in the as-prepared BZCY, which remain un-changed after H2S treatment. *Represents peak due to Ni (JCPDS card no.: 45–1027) in dry H2/30 ppm H2S treated BZCY-Ni.
The chemical stability of the as-synthesized compounds was also studied in 30 ppm H2S in a dry H2 atmosphere, with the ex situ XRD results are shown in Figure 7. After heating the BZCY, BZCY-Fe, Co, and Ni compounds in powder form at 800°C for 24 h in 30 ppm H2S balanced with dry H2, no impurity phase is observed in the BZCY-Fe and -Co samples. In the BZCY-Ni XRD pattern, however, a weak peak for metallic Ni is observed [joint committee on powder diffraction standards (JCPDS) card no.: 45–1027], which could be related to the ex-solution of Ni after reduction in dry H2 at 800°C. The BZCY synthesized in our lab showed small impurity peaks, however, after treatment in 30 ppm H2S/H2 at 800°C for 24 h no new phases were observed (Figure 7).
Previous studies of the crystal structure of BaCeO3 at a range of temperatures has shown that a transition from the space group Pnma to Imam occurs at 290°C (Knight, 1994) or 300°C (Genet et al., 1999). This transition has been identified, based on the disappearance of the 201 and 221 peaks (Genet et al., 1999), which further confirms the space group Imam. In addition to the 201 and 221 peaks, another distinct Pnma peak, which is absent, is 131 that should be just below the 221 peak. The observation of the Imam space group is interesting, as in the parent compound (BaCeO3), the occurrence of an Imam structure is triggered by the increase in temperature, while in BaZr0.1Ce0.7Y0.1M0.1O3−δ, this space group is observed at room temperature (Figure 1).
This change in crystal symmetry as a result of doping has been observed previously, where a large amount of Y3+ has replaced Ce4+ in BaCeO3 (Malavasi et al., 2008). The BaCe0.8Y0.2O3−δ compound, with 20% Y3+ doping, has been reported to have a monoclinic I2/m space group at room temperature (Malavasi et al., 2008), whereas, for BaCe0.9Y0.1O3−δ with 10% doping, a Pnma structure was reported at room temperature (Malavasi et al., 2009). The effect of doping has also been observed for Nd-doped BaCeO3 (Knight, 1999), where 5% doping has been shown to change the crystal symmetry from orthorhombic, Pnma, to tetragonal, P4/mbm, while 10% doping results in the formation of the cubic space group Pm3m. It appears that the disorder prompted by doping can lead to a similar outcome as the thermal effect. Also, the unit cell volume increases from 330.97(5) Å3 for the Fe-doped sample to 335.35(6) Å3 for the Ni-doped sample and reaches a maximum of 337.26(7) Å3 in the Yb-doped sample (Figure 1).
Effect of Dopant and Sintering Temperature on Total Conductivity and Stability in CO2
The higher conductivity of the Ni-doped sample at lower sintering temperatures, compared to other samples studied here, may be related to the higher concentration of oxygen vacancies (in air) introduced into the crystal structure upon substitution of Ni2+ at the B-site of the perovskite material. The oxygen vacancies present in the structure could be transformed to proton charge carriers (H+) upon exposure to water in wet H2 (Eq. 1). In most cases, the activation energy associated with the conductivity of these materials in air is higher than in wet H2. While it is expected that some electronic conductivity is present in both atmospheres, the lower activation energy in wet H2 could be attributed to differences in the charge carriers, i.e., protons (H+) in wet H2 compared to oxygen ions (O2−) in air. Due to their smaller size, proton transport has lower activation energy, providing a higher conductivity at lower temperatures, compared to oxygen ions.
Increasing the sintering temperature enhances the total conductivity of the BZCY-Co, as shown in Figure 8. This could be related to the formation of the Co-rich secondary phase (Figure 5H). Yang et al. (2011) have shown an increase in conductivity of the BaZr0.1Ce0.7Y0.2− xCoxO3−δ (0 ≤ x ≤ 0.2) compound with an increase in the Co content, attributing the higher conductivity values to the formation of a BaCoO3-based phase. The BaCoO3 phase has a higher electronic conductivity compared to the parent BZCY phase.
Figure 8. Effect of sintering temperature and dopant type on electrical conductivity of BZCY-M (M = Fe, Ni, and Co) at 500°C in (A) air and in (B) wet H2.
To understand the chemical composition of the secondary phase, EDX line scans were collected across the grains, with the results shown in Figure 9. The inset in Figure 9A shows that the secondary phase has a high concentration of Co, but a decreased Ce content. The Ba concentration remains almost the same in both the primary and secondary phases, suggesting the formation of a BaCoO3-based perovskite. This result is also consistent with WDS study (not shown). It has been shown that, in BaZr0.1Ce0.7Y0.2− xCoxO3−δ, a BaCoO3-based phase is observed in the XRD pattern when the Co content is about 10 mol% (Yang et al., 2011). However, in contrast to our SEM images (Figures 5H,I and 9A) that clearly show the formation of the secondary phase, XRD results (Figure 1B) do not show the BaCoO3 peaks after synthesis at 1350°C. This could be related to the lower concentration of the secondary phase in the present work. Yang et al. prepared single-phase BaZr0.1Ce0.7Y0.2− xCoxO3−δ after three times sintering and subsequent ball-milling at 1100°C for 10 h. However, in this study the BZCY-Co single-phase was obtained after firing at 1350°C. Calcination at 1350°C may have caused some Co evaporation from the compound, as blue color associated with Co was observed on the alumina crucible. This may have decreased the Co content and lowered the concentration of the BaCoO3 phase below the XRD detection limit.
Figure 9. SEM picture of (A) the surface of the BZCY-Co sample sintered at 1350°C and (B) polished surface of the BZCY-Ni sample sintered at 1550°C. The results of line scan along the white line are shown in the inset.
In contrast to the Co-doped sample, the conductivity of the BZCY-Ni compound decreases with increasing sintering temperature. At 1550°C, the sub-micron sized NiO particles can be observed at the grain-boundaries (Figure 5F), with their chemical composition confirmed by EDX analysis. A subsequent EDX line scan study on these phases confirmed that Ni and oxygen are the only elements present (Figure 9B). The ex-solution of metals at high temperatures from perovskite materials upon reduction has been reported recently (Neagu et al., 2013). This may have caused the lower conductivity of the BZCY-Ni sample after sintering at 1550°C, compared to the sample fired at two lower temperatures (Figure 8).
The enhanced tolerance of the samples fired at 1550°C toward CO2 exposure may have been caused by Ba evaporation during heat treatment at higher temperature, which makes these compounds Ba deficient and hence less prone to reaction with CO2. Although the particle size of the powders used for the two tests is very similar, the samples that were heat treated at 1550°C have larger grain sizes and fewer grain-boundaries, as shown in Figure 5.
In summary, the BZCY-Co compound, studied here, shows a very promising electrical conductivity compared to other compounds arising from the same perovskite family (Figure 10), especially at intermediate temperatures (0.01 S cm−1 at 600°C in wet H2). Thus, BZCY-Co is considered to be a very promising candidate anode material for SOFCs. The higher sintering temperature of 1550°C enhances the total conductivity of the BZCY-Co compound, due to the formation of a BaCoO3-based secondary phase. However, the highest conductivity within the BZCY-Ni samples is observed for the sample fired at the lowest sintering temperature of 1250°C. Ni ex-solution from the BZCY-Ni sample is observed after sintering at 1550°C for 12 h and seems to be responsible for the conductivity loss, as a result of bulk composition change. Also, sintering at the higher temperature of 1550°C enhances the stability of the compound in the CO2-containing environment.
Figure 10. Comparison of the reported conductivity values for barium cerate based perovskite SOFC materials in wet H2 atmosphere. In the figure, BCY 10, BZCY-Co, BZCY-Ni, BZCY-Yb, BZCY-5Co, and BZCNb represent BaCe0.9Y0.1O3−δ (Suksamai and Metcalfe, 2007; Amsif et al., 2011), BaZr0.1Ce0.7Y0.1Co0.1O3−δ sintered at 1550°C, BaZr0.1Ce0.7Y0.1Ni0.1O3−δ sintered at 1250°C, BaZr0.1Ce0.7Y0.1Yb0.1O3−δ (Yang et al., 2009), BaZr0.4Ce0.5Y0.05Co0.05O3−δ (Azimova and McIntosh, 2009), and BaZr0.1Ce0.8Nb0.1O3−δ (Bhella et al., 2011), respectively.
Conflict of Interest Statement
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
The authors would like to acknowledge financial support from the Natural Sciences and Engineering Research Council of Canada (NSERC) through the Strategic Research Network (Solid Oxide Fuel Cells Canada) Granting Program and the Institute for Sustainable Energy, Environment and Economy (ISEEE) at the University of Calgary. One of us (Behzad Mirfakhraei) is also grateful for NSERC PGSD scholarship support. We also would like to acknowledge the services of the Microscopy and Imaging Facility at the University of Calgary, access to Field-Emission SEM facilities at the University of Calgary, and Parastoo Keyvanfar for help with SEM analysis and useful discussions.
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Keywords: high temperature proton conductor, chemical stability, doped barium cerate, SOFC, anode material
Citation: Mirfakhraei B, Ramezanipour F, Paulson S, Birss V and Thangadurai V (2014) Effect of sintering temperature on microstructure, chemical stability, and electrical properties of transition metal or Yb-doped BaZr0.1Ce0.7Y0.1M0.1O3−δ (M = Fe, Ni, Co, and Yb). Front. Energy Res. 2:9. doi: 10.3389/fenrg.2014.00009
Received: 03 January 2014; Paper pending published: 30 January 2014;
Accepted: 17 February 2014; Published online: 13 March 2014.
Edited by:Fanglin Chen, University of South Carolina, USA
Reviewed by:Hongying Hou, Kunming University of Science and Technology, China
Chao Xu, North China Electric Power University, China
Shumin Fang, University of South Carolina, USA
Copyright: © 2014 Mirfakhraei, Ramezanipour, Paulson, Birss and Thangadurai. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Venkataraman Thangadurai, Department of Chemistry, University of Calgary, 2500 University Dr. NW, Calgary, AB T2N 1N4, Canada e-mail: firstname.lastname@example.org