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Enhancement of the thermoelectric power factor by tuning the carrier concentration in Cu-rich and Ge-poor colusites Cu26+xNb2Ge6-xS32
被引:4
|作者:
Bouyrie, Yohan
[1
]
Chetty, Raju
[1
]
Suekuni, Koichiro
[2
]
Saitou, Noriyuki
[3
]
Jood, Priyanka
[1
,4
]
Yoshizawa, Noriko
[3
]
Takabatake, Toshiro
[5
]
Ohta, Michihiro
[1
,4
]
机构:
[1] Natl Inst Adv Ind Sci & Technol, Res Inst Energy Conservat, Tsukuba, Ibaraki 3058568, Japan
[2] Kyushu Univ, Interdisciplinary Grad Sch Engn Sci, Dept Appl Sci Elect & Mat, Kasuga, Fukuoka 8168580, Japan
[3] Natl Inst Adv Ind Sci & Technol, Res Inst Energy Frontier, Tsukuba, Ibaraki 3058569, Japan
[4] Natl Inst Adv Ind Sci & Technol, Global Zero Emiss Res Ctr, Tsukuba, Ibaraki 3058568, Japan
[5] Hiroshima Univ, Grad Sch Adv Sci Matter, Higashihiroshima, Hiroshima 7398530, Japan
关键词:
THERMAL-CONDUCTIVITY;
EARTH-ABUNDANT;
PERFORMANCE;
TETRAHEDRITES;
CRYSTAL;
NANOCOMPOSITES;
CHEMISTRY;
TRANSPORT;
PROPERTY;
CU2SNS3;
D O I:
10.1039/d0tc00508h
中图分类号:
T [工业技术];
学科分类号:
08 ;
摘要:
Non-stoichiometric colusites Cu26+xNb2Ge6-xS32 (0 <= x <= 0.7) were prepared by mixing elemental constituents in evacuated quartz tubes at 1323 K followed by hot-pressing at 973 K. Their thermoelectric properties were investigated over the temperature range of 300 K-670 K. X-ray diffractometry and transmission electron microscopy analyses revealed that all the samples have a well crystallized structure and consist of the ordered colusite phase in which Cu, Nb, and Ge cations occupy their respective atomic positions in the structure. Energy dispersive spectroscopy analysis showed the presence of sulfur-poor and cation-rich chemical compositions in all the samples. We demonstrate that the increase of x (Cu-rich and Ge-poor) leads to an increase of the carrier concentration, resulting in a high power factor of similar to 830 mu W m(-1) K-2 at 670 K for the sample with x = 0.5. High-temperature sintering led to significant defects of sulfur and interstitial cations, which resulted in a low lattice thermal conductivity (similar to 0.4 W m(-1) K-1 at 670 K). A ZT of 0.7-0.8 was achieved at 670 K irrespective of the value of x.
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页码:6442 / 6449
页数:8
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