2017
DOI: 10.1021/acs.inorgchem.7b01584
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Prospects for Engineering Thermoelectric Properties in La1/3NbO3 Ceramics Revealed via Atomic-Level Characterization and Modeling

Abstract: A combination of experimental and computational techniques has been employed to explore the crystal structure and thermoelectric properties of A-site-deficient perovskite LaNbO ceramics. Crystallographic data from X-ray and electron diffraction confirmed that the room temperature structure is orthorhombic with Cmmm as a space group. Atomically resolved imaging and analysis showed that there are two distinct A sites: one is occupied with La and vacancies, and the second site is fully unoccupied. The diffuse sup… Show more

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Cited by 10 publications
(10 citation statements)
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References 71 publications
(159 reference statements)
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“…For example, κ total varied between 6.5 and 4 W m −1 K −1 for samples with x = 0.10, while it was almost constant at approximately 2 W m −1 K −1 for samples of x = 1.0. This temperature independence of κ total has also been reported for other A-site deficient perovskites such as, La 1/3 NbO 3 [48], Nd 2/3 TiO 3 [49,50] and Sr 1−x La 2x/3 x/3 TiO 3 [12,14]. As the microstructural features in the present investigation (figure 2) are all much larger than the phonon mean-free path (l ph ) for SrTiO 3 (less than 10 nm) [7,51], the temperature dependence of κ total cannot be linked to simple bulk microstructural effects, but can be explained by changes in crystal structure and specifically changes in lattice thermal conductivity (κ lattice ).…”
Section: (E) Thermoelectric Propertiessupporting
confidence: 81%
“…For example, κ total varied between 6.5 and 4 W m −1 K −1 for samples with x = 0.10, while it was almost constant at approximately 2 W m −1 K −1 for samples of x = 1.0. This temperature independence of κ total has also been reported for other A-site deficient perovskites such as, La 1/3 NbO 3 [48], Nd 2/3 TiO 3 [49,50] and Sr 1−x La 2x/3 x/3 TiO 3 [12,14]. As the microstructural features in the present investigation (figure 2) are all much larger than the phonon mean-free path (l ph ) for SrTiO 3 (less than 10 nm) [7,51], the temperature dependence of κ total cannot be linked to simple bulk microstructural effects, but can be explained by changes in crystal structure and specifically changes in lattice thermal conductivity (κ lattice ).…”
Section: (E) Thermoelectric Propertiessupporting
confidence: 81%
“…Finally our configurations can be thought as air sintered samples where the amount of oxygen vacancies will decrease dramatically. 50,51 All simulated systems (i.e. layered nanostructures) contain two identical grain boundaries with the X direction perpendicular to the YZ boundary plane.…”
Section: Layered Nanostructure Modelsmentioning
confidence: 99%
“…The calculations are provided at various temperatures, using a rigid-band model that assumes no shape change in the band structure, but only a shift in the Fermi energy due to the changing electron doping concentration. [5]…”
mentioning
confidence: 99%