Key Engineering Materials Vol. 566

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Abstract: ron fluoride (III) anhydrate fine particle was prepared by drying in vacuum from FeF3·3H2O, a mechanical milling process and a calcination at 473 773 K. Particle size of FeF3·3H2O was ca. 3 5 μm and that of FeF3 anhydrate was 100 500 nm after drying and milling. FeF3 sample only after drying and milling was hygroscopic and became FeF3·3H2O under atmosphere. FeF3 became stable under atmosphere after oxidation at 673 K for more than 20 minutes. It was found that Fe2O3 was produced by calcination and covered the surface of FeF3 particles. In Charge-discharge measurements, the discharge capacity of these FeF3 samples was 150 - 200 mAh/g at a discharge rate of 0.1 C. The oxidation could improve the discharge properties of FeF3 cathode.
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Abstract: Ce0.8Sm0.2O1.9 (Samaria-doped ceria: SDC) precursors were synthesized by carbon-assisted spray pyrolysis. SDC thin films were prepared by electrophoretic deposition using the SDC precursor particles. The as-prepared SDC thin films were sintered at 1600 °C for 10 h. Uniform films with a thickness of approximately 20 μm were obtained. A fuel cell using the prepared thin films showed a maximum power density of 60.6 mW/cm2 and an open circuit voltage (OCV) of 0.63 V at 700 °C.
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Abstract: All contributions to the total conductivity, electrolyteelectrode interfaces, grain boundaries, ion-hopping, and optical phonons, were determined on the 8 mol% yttria-stabilized zirconia (8YSZ) and 8 mol% ytterbia-stabilized zirconia (8YbSZ) ceramics using the wideband conductivity spectroscopy. Complex conductivity spectra from 101 Hz to 1014 Hz were successfully obtained. The higher total conductivity of the 8YbSZ ceramics compared to the 8YSZ in wideband frequencies was mainly attributed to difference in the DC conductivity due to universal dielectric response (UDR), σdc; σdc (8YbSZ) > σdc (8YSZ). Other parameters in the UDR and the optical phonon parameters did not greatly influence on the difference in their intrinsic conductivities.
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Abstract: The electrochemical capacitors (ECs) have attracted a great attention as a rechargeable strage device with a high power density and high safety. An increase in specific capacity is demanded to use ECs in various applications. MnO2 are expected as electrodes of ECs because of their large oxidation state change (Mn4+ Mn2+), low cost and environmental compatibility. When all manganese ions in the MnO2 are completely reduced to Mn2+ from Mn4+ over a potential window of 1.1 V, the theoretical capacity is estimated to about 2000 Fg-1. However, the reported capacity of MnO2 electrodes are 100250 Fg-1 [1-2] for powders and around 700 Fg-1 [3] for thin films. Tunnel structured MnO2 are expected to show high capacities by utilizing high ionic mobility in the tunnel and high surface area of tunnel walls. Fig. 1 shows crystal structures of (a) Pyrolusite (Tunnel size: 1×1), (b) Hollandite (Tunnel size: 2×2) and (c) OMS-5 (Tunnel size: 2×4) and (d) MnO6 unit. In the present study, the relationship between the tunnel size and the specific capacity was investigated for those tunnel structured MnO2. In addition, Hollandite /carbon composites were synthesized to improve the electrode properties of Hollandite.
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Abstract: We evaluated the surface area, pore size distribution, and electrical characteristics of titanium oxide films formed under different sintering and cleaning conditions. In addition, we examined the microstructure of the titanium oxide films by forming cross-sectional surfaces. The necking structure of the titanium oxide films strongly influenced the conversion efficiency of the dye-sensitized solar cell. And, the conversion efficiency was improved by the increasing firing temperature and treating with TiCl4 and ozone water.
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Abstract: The effects of processing conditions on the morphologies of Mn-doped BiFeO3 thin films have been investigated. BiFeO3 thin films were prepared on a SrTiO3 (001) substrate by CSD method. BiFeO3 grew epitaxially on SrTiO3 and Bi2Fe4O9 has also orientation relationships with BiFeO3. It was found that the formation of Bi2Fe4O9 was promoted in an O2 atmosphere. Island morphologies were observed in the BiFeO3 thin films after post-annealing at 1023K both in N2 and O2 atmospheres. The formation of the islands is promoted in an O2 atmosphere.
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Abstract: Ferroelectric 0.7BiFeO3-0.3BaTiO3 and 0.7BiFe0.95Mn0.05O3-0.3BaTiO3 thin films were prepared by the chemical solution deposition. Perovskite single-phase thin films with homogeneous surface morphology were successfully fabricated at 700°C on Pt/TiOx/SiO2/Si substrates. Although typical polarization (P)-electric field (E) hysteresis loops were observed for 0.7BiFeO3-0.3BaTiO3 thin films, their insulation resistance was relatively low at room temperature. Mn doping for Fe site of the 0.7BiFeO3-0.3BaTiO3 was very effective in improving leakage current properties. In 0.7BiFe0.95Mn0.05O3-0.3BaTiO3 thin films, the abrupt increase in leakage current was suppressed even at high electric fields, leading to the well-shaped P-E hysteresis loops at ambient temperatures. Remanent polarization and coercive field of the 0.7Bi (Fe0.95Mn0.05)O3-0.3Bi0.5Na0.5TiO3 films at room temperature were approximately 26 μC/cm2 and 130 kV/cm, respectively.
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Abstract: Bi-based perovskite-type oxide materials such as BiFeO3 (BFO) and Bi (Zn1/2Ti1/2)O3 and the related compounds receive much attention and have been developed actively as important candidates for Pb-free ferroelectric materials instead of toxic Pb-based perovskite oxide materials. Recently, many researches have been reported for thin films of Bi-based materials by various film-deposition techniques for actual application of semiconductive devices, microactuators, etc. In this study, we tried preferential crystal growth of BFZT films on semiconductive silicon substrates using uniaxial-(100)-oriented LaNiO3 (LNO) buffer layer. BFO films were fabricated via chemical solution deposition (CSD) technique on platinized silicon wafer [(111)Pt/TiO2/(100)S and (100)LNO-coated platinized silicon [(100)LNO/(111)Pt/TiO2/(100)S substrates. XRD analysis indicated that the films fabricated on (111)Pt/TiO2/(100)Si substrate consisted of randomly-oriented BFZT crystal with lower crystallinity. On the other hand, the films on (100)LNO/(111)Pt/TiO2/(100)Si consisted of uniaxial-one-oriented BFZT crystal with higher crystallinity. The crystallization temperature these films were 500°C, respectively. These results suggest that the BFZT crystal was grown successfully on uniaxial oriented (100)LNO plane which also had perovskite-type crystal structure. Consequently, one-oriented BFZT films were prepared on Si substrate successfully using (100)LNO buffer layer.
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Abstract: We have elucidated the elastic interaction between the 90° domains and misfit dislocations in PbTiO3/SrTiO3 (001) epitaxial thin films by the local strain mapping based on high-resolution transmission electron microscopy. The novel mechanism of the nucleation and growth of 90 ̊ domain has been proposed based on the results, including the introduction of the additional dislocation perpendicular to the misfit dislocation and the dissociation of these dislocations into two pairs of partial dislocations with an anti-phase boundary.
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Abstract: The microstructure of an epitaxial PbTiO3 thick film was investigated by using transmission electron microscopy (TEM). An analysis of bright-field TEM (BFTEM) images revealed the existence of displacements along the [00 direction of PbTiO3. High-resolution TEM (HRTEM) observation indicated that stacking faults parallel to the (001) plane of PbTiO3 are formed in the thick film. Local strain fields around the stacking faults were quantified by geometric phase analysis of the HRTEM image. The measured strain suggested the presence of a pair of extrinsic and intrinsic stacking faults. The distance between an extrinsic stacking fault and an intrinsic one corresponds to two unit cells along the [00 direction of PbTiO3. The formation of these stacking faults is considered to be associated with the strain relaxation of the film.
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