TY - JOUR
T1 - Transport, magnetic, thermoelectric, and structural properties of hollandite titanates BaxTi8 O16+δ
AU - Yamashita, Y.
AU - Okuda, T.
AU - Mori, S.
AU - Horibe, Y.
AU - Murata, R.
AU - Katsufuji, T.
N1 - Funding Information:
We thank D. Araki and T. Yano for their help with the experiment and T. Mizokawa for the fruitful discussion. This work was supported by JST CREST Grant No. JPMJCR15Q2 and by JSPS KAKENHI Grant No. 16H04020.
Publisher Copyright:
© 2018 American Physical Society.
PY - 2018/7/30
Y1 - 2018/7/30
N2 - We studied hollandite titanates BaxTi8O16+δ, which have double chains of edge-sharing TiO6 octahedra with various numbers of d electrons per Ti n=(x-δ)/4. Anomalies at ∼200K were observed in the temperature dependence of various quantities over a wide range of n, which were caused by the charge ordering of the d electrons. It was found that charge ordering is stable when d electrons exist at every fifth site along the Ti chain. A structural phase transition from tetragonal to monoclinic occurs as a secondary effect of the charge ordering. When n is close to 0.4, the anomalies at ∼200K disappear, and the crystal structure remains monoclinic from 300 K down to the lowest temperatures. It was also found that this series of compounds exhibits negative Seebeck coefficients with large absolute values at room temperature and that the figure of merit for thermoelectric materials (ZT) was maximized at n∼0.22 (0.05 at room temperature).
AB - We studied hollandite titanates BaxTi8O16+δ, which have double chains of edge-sharing TiO6 octahedra with various numbers of d electrons per Ti n=(x-δ)/4. Anomalies at ∼200K were observed in the temperature dependence of various quantities over a wide range of n, which were caused by the charge ordering of the d electrons. It was found that charge ordering is stable when d electrons exist at every fifth site along the Ti chain. A structural phase transition from tetragonal to monoclinic occurs as a secondary effect of the charge ordering. When n is close to 0.4, the anomalies at ∼200K disappear, and the crystal structure remains monoclinic from 300 K down to the lowest temperatures. It was also found that this series of compounds exhibits negative Seebeck coefficients with large absolute values at room temperature and that the figure of merit for thermoelectric materials (ZT) was maximized at n∼0.22 (0.05 at room temperature).
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U2 - 10.1103/PhysRevMaterials.2.074409
DO - 10.1103/PhysRevMaterials.2.074409
M3 - Article
AN - SCOPUS:85058027605
SN - 2475-9953
VL - 2
JO - Physical Review Materials
JF - Physical Review Materials
IS - 7
M1 - 074409
ER -