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Acta Metall Sin  2023, Vol. 59 Issue (2): 237-247    DOI: 10.11900/0412.1961.2021.00215
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Thermoelectric Properties of P-Type CeyFe3CoSb12 Thermoelectric Materials and Coatings Doped with La
LI Dou, XU Changjiang, LI Xuguang, LI Shuangming(), ZHONG Hong
State Key Laboratory of Solidification Processing, Northwestern Polytechnical University, Xi'an 710072, China
Cite this article: 

LI Dou, XU Changjiang, LI Xuguang, LI Shuangming, ZHONG Hong. Thermoelectric Properties of P-Type CeyFe3CoSb12 Thermoelectric Materials and Coatings Doped with La. Acta Metall Sin, 2023, 59(2): 237-247.

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Abstract  

During the use of fossil fuels, about two-thirds of the energy that is discharged into the environment in the form of waste heat are barely utilized and cause considerable environmental pollution and intense CO2 emission. Thermoelectric materials directly convert heat energy to electricity, thus, improving the utilization efficiency of fossil energy and reducing environmental pollution. Skutterudite CoSb3 has been widely studied as one of the materials for thermoelectric applications in the middle-temperature region. CoSb3-based skutterudites are narrow bandgap semiconductors with a high-electrical conductivity and Seebeck coefficient. Meanwhile, thermoelectric performance of bulk CoSb3 has been considerably improved via doping and design of nano structures. Herein, P-type CoSb3 was synthesized via melt-annealing-spark plasma sintering process. The effect of Ce-doping content on microstructure and thermoelectric properties of CoSb3 and the effect of La doping on decoupled thermoelectric performance were studied. Compared with Ce0.8Fe3CoSb12, the Seebeck coefficient of La0.1Ce0.8Fe3CoSb12 increased with temperature, electrical resistivity decreased from 25 μΩ·m to 15 μΩ·m at 300 K, and power factor simultaneously increased from 480 μW/(m·K2) to 642 μW/(m·K2) at 673 K. The La0.1Ce0.8Fe3CoSb12 thermal conductivity decreased with La or Ce doping to ~1 W/(m·K), and the corresponding thermoelectric figure of merit reached 0.45 at 723 K in the temperature range from 300 K to 723 K. Al-Ni coating was deposited on the sintered bulk skutterudite via magnetron sputtering method. It was demonstrated that the coating did not degrade the thermoelectric performance, while the coating elements were uniformly distributed across the sintered bulk La0.1Ce0.8Fe3CoSb12. The welding behavior of P-type La0.1Ce0.8Fe3CoSb12 was studied using a Ag40Cu60 solder and a Mo50Cu50 electrode sheet. The interface of this thermoelectric material was prone to cracking and pore formation, while the elements at the interface have not demonstrated remarkable diffusion. This indicates an efficiency of the interface bonding, which may be used in the fabrication technologies of thermoelectric devices.

Key words:  CoSb3      thermoelectric material      Al-Ni coating      thermal conductivity      electrical conductivity     
Received:  19 May 2021     
ZTFLH:  TQ174  
Fund: National Natural Science Foundation of China(51774239)
About author:  LI Shuangming, professor, Tel: (029)88493264, E-mail: lsm@nwpu.edu.cn

URL: 

https://www.ams.org.cn/EN/10.11900/0412.1961.2021.00215     OR     https://www.ams.org.cn/EN/Y2023/V59/I2/237

Fig.1  XRD spectra of LaxCeyFe3CoSb12 thermoelectric material before (a) and after (b) spark plasma sintering (SPS)
Fig.2  SEM image (a) and corresponding EDS maps (b-f) of the SPSed bulk La0.1Ce0.8Fe3CoSb12 thermoelectric material
PointCoSbFeCeLaTotal
11.5673.5524.770.120.00100
23.4368.5019.017.301.76100
36.4173.2616.672.940.72100
45.7371.9518.033.141.15100
Table 1  EDS analysis results of points 1-4 in Fig.2a
Fig.3  Electrical performance curves of the SPSed bulk LaxCeyFe3CoSb12 thermoelectric material
(a) Seebeck coefficient
(b) electrical resistivity
(c) power factor
CompoundHallCarrierCarrier
coefficientmobilityconcentration
10-2 cm·C-1cm2·V-1·s-11020 cm-3
Ce0.8Fe3CoSb121.636.133.83
Ce0.9Fe3CoSb122.5258.302.48
La0.1Ce0.8Fe3CoSb123.5824.301.74
Table 2  Electrical properties of the SPSed bulk LaxCey-Fe3CoSb12 thermoelectrical material at room temperature
Fig.4  Heat transport performance curves of the SPSed bulk LaxCeyFe3CoSb12 thermoelectric material
(a) total thermal conductivity (Kt) (b) lattice thermal conductivity (KL)
(c) carrier thermal conductivity (Ke) (d) the ratio of KL / Kt
Fig.5  TEM analyses of the SPSed bulk La0.1Ce0.8Fe3CoSb12 thermoelectric material
(a) low-magnification bright-field TEM image (b) enlarged view of boxed region b in Fig.5a
(c) bright-field TEM image of grain boundary (d) EDS maps of element distribution for Fig.5c
(e) HRTEM image corresponding to region e in Fig.1a (Inset shows the SAED pattern)
(f) inverse fast Fourier transformation (IFFT) image using the satellite spots in the inset of Fig.5e (CeSb/(01ˉ1))
(g) IFFT image using the satellite spots in the inset of Fig.5e (CoSb3/(1ˉ11ˉ))
Fig.6  Thermoelectric figure of merit (ZT) of the SPSed bulk LaxCeyFe3CoSb12 thermoelectric material
Fig.7  Characterizations and analyses of the SPSed bulk La0.1Ce0.8Fe3CoSb12 thermoelectric material with sputtering Al-Ni coating
(a) photo before and after sputtering Al-Ni coating
(b) OM image of substrate and coating
(c) SEM image of coating (d, e) EDS maps of elements Al (d) and Ni (e) of rectangle area in Fig.7c (f) SEM image of substrate and coating (g) line scan result along line EF in Fig.7f
Fig.8  Thermoelectric properties curves of the SPSed bulk La0.1Ce0.8Fe3CoSb12 thermoelectric material before and after sputtering Al-Ni coating
(a) Seebeck coefficient (b) electrical resistivity
(c) thermal conductivity (d) thermoelectric figure of merit
Fig.9  SEM image of the SPSed bulk La0.1Ce0.8Fe3CoSb12 thermoelectric material joint (a) and the line scan result along line AB in Fig.9a (b)
Fig.10  SEM image of the SPSed bulk La0.1Ce0.8Fe3CoSb12 thermoelectric material after welding and corresponding elements distribution
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