“…The Raman spectra of the powders derived from the solution of pH 14 and 15 are almost the same, which are similar to that of HT-Sr 4 Nb 2 O 9 reported by Levin and Julia [14], but they are different from those of the powders synthesized at pH 12 or 13. When pH value 14 or 15, four resonance peaks are observed at 810, 580, 420 and 320 cm −1 (the last three peaks are broad and there locations can be determined only approximately).…”
Section: Structural Characterizationsupporting
confidence: 76%
“…5 and 6, respectively. The Raman spectra of the powders derived from the solution of pH 12 or 13 show two bands in the nondegenerate symmetric region (700-1000 cm −1 ) at 790 cm −1 (strong) and 860 cm −1 (weak), corresponding to Nb-O stretching vibrations [14,15]. Another strong mode at 310 cm −1 is assigned to the symmetric stretching octahedral internal mode [16].…”
Section: Structural Characterizationmentioning
confidence: 98%
“…This is in reasonable agreement with the expected com- position of the new phase Ba 4 Nb 2 O 9 . Indexing the XRD spectra of the new compound yields an average cubic structure (Fm3m, a ≈ 2a c , where "c" refers to the cubic perovskite unit cell) with 1:1 (NaCl-type) partial ordering of Ba 2+ and Nb 5+ on the Bsites like the high-temperature polymorph of Sr 4 Nb 2 O 9 [14]. Fig.…”
“…The Raman spectra of the powders derived from the solution of pH 14 and 15 are almost the same, which are similar to that of HT-Sr 4 Nb 2 O 9 reported by Levin and Julia [14], but they are different from those of the powders synthesized at pH 12 or 13. When pH value 14 or 15, four resonance peaks are observed at 810, 580, 420 and 320 cm −1 (the last three peaks are broad and there locations can be determined only approximately).…”
Section: Structural Characterizationsupporting
confidence: 76%
“…5 and 6, respectively. The Raman spectra of the powders derived from the solution of pH 12 or 13 show two bands in the nondegenerate symmetric region (700-1000 cm −1 ) at 790 cm −1 (strong) and 860 cm −1 (weak), corresponding to Nb-O stretching vibrations [14,15]. Another strong mode at 310 cm −1 is assigned to the symmetric stretching octahedral internal mode [16].…”
Section: Structural Characterizationmentioning
confidence: 98%
“…This is in reasonable agreement with the expected com- position of the new phase Ba 4 Nb 2 O 9 . Indexing the XRD spectra of the new compound yields an average cubic structure (Fm3m, a ≈ 2a c , where "c" refers to the cubic perovskite unit cell) with 1:1 (NaCl-type) partial ordering of Ba 2+ and Nb 5+ on the Bsites like the high-temperature polymorph of Sr 4 Nb 2 O 9 [14]. Fig.…”
“…As the growth temperature deviated from the optimal value, the resistivity drastically increased, probably owing to the off-stoichiometry mentioned previously: Excess oxygen layers introduced at lower growth temperatures compensate the electron carriers and suppress their mobility by breaking up the NbO 6 octahedral network. At higher growth temperatures, though, other defects are generated, such as Nb vacancies and Sr substitutions in the B site [20], both of which increase the Nb valence from 4+ to 5+ and thus decrease the carrier density. Figure 4 plots the resistivity and mobility of the stoichiometric SrNbO 3 epitaxial thin film as functions of temperature.…”
), the reported electrical resistivity of SrNbO 3 is much higher than that of SrVO 3 , probably owing to nonstoichiometry. In this paper, we grew epitaxial, high-conductivity stoichiometric SrNbO 3 using pulsed laser deposition. The growth temperature strongly affected the Sr/Nb ratio and the oxygen content of the films, and we obtained stoichiometric SrNbO 3 at a very narrow temperature window around 630 °C. The stoichiometric SrNbO 3 epitaxial thin films grew coherently on KTaO 3 (001) substrates with high crystallinity. The room-temperature resistivity of the stoichiometric film was 2.82 × 10 −5 cm, one order of magnitude lower than the lowest reported value of SrNbO 3 and comparable with that of SrVO 3 . We observed a T-square dependence of resistivity below T* = 180 K and non-Drude behavior in near-infrared absorption spectroscopy, attributable to the Fermi-liquid nature caused by electron correlation. Analysis of the T-square coefficient A of resistivity experimentally revealed that the 4d orbital of Nb that is larger than the 3d ones certainly contributes to the high electrical conduction of SrNbO 3 .
“…The capacitances obtained for barium zirconate and strontium niobate are in the same order of magnitude as for ZrO 2 . These correspond to lower than expected k-values (~15 for barium zirconate, ~19 for strontium niobate, extracted from thickness series not shown here) compared to bulk material and thick film properties [13,14]. This can be explained by thickness effects [15], the amorphous character and possible interfacial reactions on SiO x /Si substrates [11] and thus leaves room for optimization in the deposition process.…”
Section: Figure 4 A) Room Temperature Xrd Of Zro 2 /Pt Films (~5 Nm) mentioning
Important material properties of dielectric oxide films fabricated by aqueous chemical solution deposition, such as crystallization, topography, contamination and interfacial layer were evaluated and related to the films' dielectric properties.Functional ultrathin films (<20 nm thickness) of zirconia, barium zirconate and strontium niobate were deposited. These films were all subjected to the same pyrolysis treatment, based on the high similarity of their precursors' thermal decomposition behavior. The evolution of the chemical purity as a function of temperature and the effect of annealing on the interfacial SiO 2 layer was studied by grazing angle ATR-FTIR. The crystallization behavior was dependent on film thickness and composition as shown by high temperature XRD. C-V characterization demonstrated a k-value in the same order of magnitude as for the ZrO 2 reference material. This is lower than the bulk material's value, thus leaving room for further optimization of the current materials or alternatively selection of other material compositions.
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