Thermoelectric Optimization of n-Type AgBiSe2 via Se Vacancy Control and Transition-Metal Doping
Source abstract
Abstract
Silver bismuth selenide (AgBiSe 2 ) has garnered attention as a Pb-free material with a high thermoelectric efficiency owing to its intrinsically low thermal conductivity. Although pristine AgBiSe 2 is an n-type material, in this study, a weak p-type intrinsic property is achieved in AgBiSe 2 owing to the high sensitivity of its carrier type and concentration to Se vacancies. Herein, we report the enhancement of the thermoelectric performance of AgBiSe 2 by introducing Se vacancies and aliovalent transition-metal doping at the Ag site. Se vacancies are first introduced to switch the conductivity of AgBiSe 2 to the n-type and considerably increase the carrier concentration. Further, aliovalent transition-metal dopants are incorporated to tune the carrier concentration and thus increase the electrical conductivity of AgBiSe 2 . The electrical mobility and effective mass are also increased, which improves the electrical properties and enhances the power factor. The Ag 0.97 Cd 0.03 BiSe 1.995 sample exhibited the highest dimensionless figure of merit ( zT max ) of ∼0.65 at 773 K and an average dimensionless zT avg of ∼0.39 between 323 and 773 K.
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
Department of Mechanical Engineering, The University of Hong Kong, Pokfulam Road, Hong Kong SAR, China
School of Physical Sciences, Great Bay University, Dongguan 523000, China
Funding
Research Grants Council, University Grants Committee
References (31)
Show source-provided references
1. 10.1021/acs.chemrev.0c0002610.1021/acs.chemrev.0c00026 ↗
2. 10.1016/j.nantod.2018.04.00210.1016/j.nantod.2018.04.002 ↗
3. 10.1088/1755-1315/434/1/01201410.1088/1755-1315/434/1/012014 ↗
4. Ibach H. · 2012
5. 10.1016/j.actamat.2014.12.04210.1016/j.actamat.2014.12.042 ↗
6. Goldsmid H. J. · 2016 · 12110.1007/978-3-662-49256-7 ↗
7. 10.1063/5.011532210.1063/5.0115322 ↗
8. Slack G. A. · 1995
9. 10.1021/jacs.0c0771210.1021/jacs.0c07712 ↗
10. 10.1021/acsenergylett.1c0045010.1021/acsenergylett.1c00450 ↗
11. 10.1039/D1EE02986J10.1039/D1EE02986J ↗
12. 10.1038/s41535-018-0127-y10.1038/s41535-018-0127-y ↗
13. 10.1021/jacs.0c0706710.1021/jacs.0c07067 ↗
14. 10.1038/s41563-021-01064-610.1038/s41563-021-01064-6 ↗
15. 10.1002/adma.20220372510.1002/adma.202203725 ↗
16. 10.26599/JAC.2023.922074010.26599/JAC.2023.9220740 ↗
17. 10.1039/C9TA00475K10.1039/C9TA00475K ↗
18. 10.1002/aenm.20200330410.1002/aenm.202003304 ↗
19. 10.1039/C7RA12819C10.1039/C7RA12819C ↗
20. 10.1039/C4TA04912H10.1039/C4TA04912H ↗
21. 10.1039/C7DT04821A10.1039/C7DT04821A ↗
22. 10.1002/crat.20170007510.1002/crat.201700075 ↗
23. 10.1063/1.496377910.1063/1.4963779 ↗
24. 10.1021/ja312474n10.1021/ja312474n ↗
25. 10.1002/adfm.20190840510.1002/adfm.201908405 ↗
26. 10.1016/j.mtphys.2019.10010210.1016/j.mtphys.2019.100102 ↗
27. 10.1002/advs.20220378210.1002/advs.202203782 ↗
28. 10.1039/D3EE01226C10.1039/D3EE01226C ↗
29. 10.1126/science.adg719610.1126/science.adg7196 ↗
30. 10.1002/anie.20180984110.1002/anie.201809841 ↗
31. 10.1016/j.actamat.2017.09.02910.1016/j.actamat.2017.09.029 ↗