Ti-Doped CuGaTe2 as a High-Performance Thermoelectric Material: Enhancing Thermoelectric Properties through N-Type Doping
Source abstract
Abstract
CuGaTe 2 has attracted significant attention as a promising thermoelectric material due to its high Seebeck coefficient and moderate band gap. However, its intrinsic low carrier concentration and electrical conductivity limit the further enhancement of its thermoelectric performance. While most research has focused on p-type doping to increase hole carriers, excessive p-type doping can lead to carrier compensation effects, with some dopant atoms occupying Cu sites, thus weakening the doping effect. As a result, studies on n-type doping of CuGaTe 2 are relatively scarce. This study investigates the effects of n-type doping in CuGaTe 2 by introducing Ti as an n-type dopant, which effectively increases the electron carrier concentration. First-principles calculations and experimental results show that appropriate Ti doping not only improves the electrical transport properties but also significantly reduces the lattice thermal conductivity, leading to a notable increase in the ZT value. This research demonstrates that n-type doping can also improve the thermoelectric performance of CuGaTe 2 to some extent, providing insights for doping optimization in CuGaTe 2 .
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Advanced Thermoelectric Materials and Devices · Chalcogenide Semiconductor Thin Films · Quantum Dots Synthesis And Properties
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
School of Materials Science and Engineering
Xiamen University of Technology
College of New Energy and Materials
China University of Petroleum
Funding
Natural Science Foundation of Fujian Province · National Natural Science Foundation of China
References (37)
Show source-provided references
1. 10.1002/adfm.20242337110.1002/adfm.202423371 ↗
2. 10.1021/acsenergylett.4c0068010.1021/acsenergylett.4c00680 ↗
3. 10.1039/D3MH01646C10.1039/D3MH01646C ↗
4. 10.1038/nmat209010.1038/nmat2090 ↗
5. 10.1179/09506600322501018210.1179/095066003225010182 ↗
6. 10.1063/1.88175210.1063/1.881752 ↗
7. 10.1002/anie.20060237310.1002/anie.200602373 ↗
8. 10.1126/science.aad192010.1126/science.aad1920 ↗
9. 10.1088/1674-1056/27/4/04840310.1088/1674-1056/27/4/048403 ↗
10. 10.1093/nsr/nwaa25910.1093/nsr/nwaa259 ↗
11. 10.1016/j.rser.2017.10.11210.1016/j.rser.2017.10.112 ↗
12. 10.1002/adfm.20090126110.1002/adfm.200901261 ↗
13. 10.1002/smll.20210132810.1002/smll.202101328 ↗
14. 10.1021/nl203485910.1021/nl2034859 ↗
15. 10.1126/science.115972510.1126/science.1159725 ↗
16. 10.1038/s41535-018-0127-y10.1038/s41535-018-0127-y ↗
17. 10.1002/adma.20160588710.1002/adma.201605887 ↗
18. 10.1016/j.joule.2020.03.00410.1016/j.joule.2020.03.004 ↗
19. 10.1002/adma.20180707110.1002/adma.201807071 ↗
20. 10.1039/C6TC02501C10.1039/C6TC02501C ↗
21. 10.1016/j.joule.2018.02.01610.1016/j.joule.2018.02.016 ↗
22. 10.1002/adma.20120073210.1002/adma.201200732 ↗
23. 10.1103/PhysRevB.28.582210.1103/PhysRevB.28.5822 ↗
24. 10.1146/annurev.matsci.27.1.62510.1146/annurev.matsci.27.1.625 ↗
25. 10.1016/j.tsf.2004.11.04210.1016/j.tsf.2004.11.042 ↗
26. 10.1063/1.165553710.1063/1.1655537 ↗
27. 10.1021/acsaem.0c0238610.1021/acsaem.0c02386 ↗
28. 10.1021/acsami.4c0045510.1021/acsami.4c00455 ↗
29. 10.1016/j.cej.2021.13180710.1016/j.cej.2021.131807 ↗
30. 10.1021/acs.chemmater.4c0142710.1021/acs.chemmater.4c01427 ↗
31. 10.1002/aesr.20230006910.1002/aesr.202300069 ↗
32. 10.1039/C5TC03325J10.1039/C5TC03325J ↗
33. 10.1016/j.jmat.2018.02.00210.1016/j.jmat.2018.02.002 ↗
34. 10.1016/j.ssc.2022.11483610.1016/j.ssc.2022.114836 ↗
35. 10.1039/c4ra02595d10.1039/c4ra02595d ↗
36. 10.1016/j.jallcom.2024.17496110.1016/j.jallcom.2024.174961 ↗
37. 10.1038/s41524-021-00587-510.1038/s41524-021-00587-5 ↗