TY - JOUR
T1 - Thermal Transport Properties of a Mixed Anion Layered Compound, Polycrystalline LaCu1-δS0.5Se0.5O (δ = 0.01)
AU - Azuma, Nobuhiko
AU - Sawada, Hiroki
AU - Ito, Hirotaka
AU - Sakagami, Ryosuke
AU - Tanaka, Yuya
AU - Fujioka, Tatsuhide
AU - Matoba, Masanori
AU - Kamihara, Yoichi
N1 - Publisher Copyright:
© Materials Research Society of Korea, All rights reserved. This is an Open-Access article distributed under the terms of the Creative Commons Attribution Non-Commercial License (https://creativecommons.org/licenses/by-nc/4.0/) which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.
PY - 2024
Y1 - 2024
N2 - Electrical and thermal transport properties of a polycrystalline carrier-doped wide-gap semiconductor LaCu1-δ S0.5Se0.5O (δ = 0.01), in which the CuCh (Ch = S, Se) layer works as conducting layer, were measured at temperatures 473~673 K. The presence of δ = 0.01 copper defects dramatically reduces the electrical resistivity (ρ) to approximately one part per million compared to that of δ = 0 at room temperature. The polycrystalline δ = 0.01 sample exhibited ρ of 1.3 × 10-3 Ωm, thermal conductivity of 6.0 Wm-1 K-1, and Seebeck coefficient (S) of 87 µVK-1 at 673 K. The maximum value of the dimensionless figure of merit (ZT) of the δ = 0.01 sample was calculated to be 6.4 × 10-4 at T = 673 K. The ZT value is far smaller than a ZT ~ 0.01 measured for a nominal LaCuSeO sample. The smaller ZT is mainly due to the small S measured for LaCu1-δS0.5Se0.5O (δ = 0.01). According to the Debye model, above 300 K phonon thermal conductivity in a pure lattice is inversely proportional to T, while thermal conductivity of the δ = 0.01 sample increases with increasing T.
AB - Electrical and thermal transport properties of a polycrystalline carrier-doped wide-gap semiconductor LaCu1-δ S0.5Se0.5O (δ = 0.01), in which the CuCh (Ch = S, Se) layer works as conducting layer, were measured at temperatures 473~673 K. The presence of δ = 0.01 copper defects dramatically reduces the electrical resistivity (ρ) to approximately one part per million compared to that of δ = 0 at room temperature. The polycrystalline δ = 0.01 sample exhibited ρ of 1.3 × 10-3 Ωm, thermal conductivity of 6.0 Wm-1 K-1, and Seebeck coefficient (S) of 87 µVK-1 at 673 K. The maximum value of the dimensionless figure of merit (ZT) of the δ = 0.01 sample was calculated to be 6.4 × 10-4 at T = 673 K. The ZT value is far smaller than a ZT ~ 0.01 measured for a nominal LaCuSeO sample. The smaller ZT is mainly due to the small S measured for LaCu1-δS0.5Se0.5O (δ = 0.01). According to the Debye model, above 300 K phonon thermal conductivity in a pure lattice is inversely proportional to T, while thermal conductivity of the δ = 0.01 sample increases with increasing T.
KW - Cu defect
KW - OSSeO.
KW - mixed anion layered compounds
KW - thermoelectric material
UR - https://www.scopus.com/pages/publications/85211157353
UR - https://www.scopus.com/pages/publications/85211157353#tab=citedBy
U2 - 10.3740/MRSK.2024.34.10.464
DO - 10.3740/MRSK.2024.34.10.464
M3 - Article
AN - SCOPUS:85211157353
SN - 1225-0562
VL - 34
SP - 464
EP - 474
JO - Korean Journal of Materials Research
JF - Korean Journal of Materials Research
IS - 10
ER -