TY - JOUR
T1 - Thermoelectric properties of LiCo1-xMxO2 (M = Cu, Mg, Ni, Zn)
T2 - Comparison with LiyCoO2 and NayCoO2 systems
AU - Mizuno, Shu
AU - Fujishiro, Hiroyuki
AU - Ishizawa, Mamoru
AU - Naito, Tomoyuki
AU - Katsui, Hirokazu
AU - Goto, Takashi
N1 - Publisher Copyright:
© 2017 The Japan Society of Applied Physics.
PY - 2017/2
Y1 - 2017/2
N2 - LiyCoO2 has a similar layered structure to NayCoO2, which is a typical p-type oxide thermoelectric material, and the average Co valence of 3 + y is controlled by the Li content y. We investigated the thermoelectric properties of LiCo1-xMxO2 samples (M = Cu, Mg, Ni, Zn) for the first time at high temperatures, in which Co3+ was substituted by the divalent M2+ ions, and the average Co valence of 3 + x can be controlled similarly to the Li content y in LiyCoO2. The substitution of the M2+ ions for the Co site was found to show thermoelectric properties similar to those of LiyCoO2 with the same average Co valence. The Mg-doped sample showed the highest thermoelectric performance at high temperatures in this study; the thermoelectric power factor P is 2.38 × 10-4 W m-1 K-2 at 1173 K and the dimensionless figure of merit ZT is 0.024 at 876 K. The thermoelectric potential of LiCo1-xMxO2 is discussed and compared with those of LiyCoO2 and NayCO2 systems.
AB - LiyCoO2 has a similar layered structure to NayCoO2, which is a typical p-type oxide thermoelectric material, and the average Co valence of 3 + y is controlled by the Li content y. We investigated the thermoelectric properties of LiCo1-xMxO2 samples (M = Cu, Mg, Ni, Zn) for the first time at high temperatures, in which Co3+ was substituted by the divalent M2+ ions, and the average Co valence of 3 + x can be controlled similarly to the Li content y in LiyCoO2. The substitution of the M2+ ions for the Co site was found to show thermoelectric properties similar to those of LiyCoO2 with the same average Co valence. The Mg-doped sample showed the highest thermoelectric performance at high temperatures in this study; the thermoelectric power factor P is 2.38 × 10-4 W m-1 K-2 at 1173 K and the dimensionless figure of merit ZT is 0.024 at 876 K. The thermoelectric potential of LiCo1-xMxO2 is discussed and compared with those of LiyCoO2 and NayCO2 systems.
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U2 - 10.7567/JJAP.56.021101
DO - 10.7567/JJAP.56.021101
M3 - Article
AN - SCOPUS:85011565806
VL - 56
JO - Japanese Journal of Applied Physics, Part 1: Regular Papers & Short Notes
JF - Japanese Journal of Applied Physics, Part 1: Regular Papers & Short Notes
SN - 0021-4922
IS - 2
M1 - 021101
ER -