Enhanced Transverse Seebeck Coefficients in 2D/2D PtSe2/MoS2 Heterostructures Using Wet-Transfer Stacking
Source abstract
Abstract
It is very challenging to estimate thermoelectric (TE) properties when applying millimeter-scale two-dimensional (2D) transition metal dichalcogenide (TMDC) materials to TE device applications, particularly their Seebeck coefficient due to their high intrinsic electrical resistance. This paper proposes an innovative approach to measure large transverse (i.e., in-plane) Seebeck coefficients for 2D TMDC materials by placing a low resistance (LR) semimetallic PtSe2 film on high-resistance (HR) semiconducting MoS2 (>10 MΩ), whose internal resistance is too high to measure the Seebeck coefficient, forming a heterojunction structure using wet-transfer stacking. The vertically stacked LR-PtSe2 (3 nm)/HR-MoS2 (12 nm) heterostructure film exhibits a high Seebeck coefficient > 190 μV/K up to 5 K temperature difference. This unusual behavior can be explained by an additional Seebeck effect induced at the interface between the LR-2D/HR-2D heterostructure. The proposed stacked LR-PtSe2/HR-MoS2 heterostructure film offers promising phenomena 2D/2D materials that enable innovative TE device applications.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Advanced Thermoelectric Materials and Devices · 2D Materials and Applications · Thermal properties of materials
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Physics and Center for Berry Curvature Based New Phenomena, Chung-Ang University, Seoul06974, Republic of Korea
Division of Solid-State Electronics, Department of Electrical Engineering, Uppsala University, Uppsala75103, Sweden
Funding
Samsung Science and Technology Foundation · National Research Foundation of Korea
References (35)
Show source-provided references
1. 10.1103/PhysRevB.94.01431210.1103/PhysRevB.94.014312 ↗
2. 10.1038/s41535-018-0083-610.1038/s41535-018-0083-6 ↗
3. 10.1103/PhysRevB.95.11540710.1103/PhysRevB.95.115407 ↗
4. 10.1088/0957-4484/27/37/37570310.1088/0957-4484/27/37/375703 ↗
5. 10.1039/C6TA10219K10.1039/C6TA10219K ↗
6. 10.1038/s41467-018-03436-010.1038/s41467-018-03436-0 ↗
7. 10.1039/C6TC03074B10.1039/C6TC03074B ↗
8. 10.1021/acsnano.9b0652310.1021/acsnano.9b06523 ↗
9. 10.1021/acs.chemmater.0c0435110.1021/acs.chemmater.0c04351 ↗
10. 10.1126/science.119497510.1126/science.1194975 ↗
11. 10.1016/j.nanoen.2016.05.02210.1016/j.nanoen.2016.05.022 ↗
12. 10.1021/nl303321g10.1021/nl303321g ↗
13. 10.1021/acsnano.2c0035910.1021/acsnano.2c00359 ↗
14. 10.1039/C7CS00880E10.1039/C7CS00880E ↗
15. 10.1103/PhysRevLett.110.06720710.1103/PhysRevLett.110.067207 ↗
16. 10.1088/0953-8984/26/34/34320210.1088/0953-8984/26/34/343202 ↗
17. 10.1126/science.117124510.1126/science.1171245 ↗
18. 10.1039/D1TA07854B10.1039/D1TA07854B ↗
19. 10.1103/PhysRevB.59.175810.1103/PhysRevB.59.1758 ↗
20. 10.1103/PhysRevLett.77.386510.1103/PhysRevLett.77.3865 ↗
21. 10.1103/PhysRevB.92.16542610.1103/PhysRevB.92.165426 ↗
22. 10.1016/j.physleta.2016.09.01510.1016/j.physleta.2016.09.015 ↗
23. 10.1021/acsami.9b0107810.1021/acsami.9b01078 ↗
24. 10.1039/D0TA06846B10.1039/D0TA06846B ↗
25. 10.1039/D0TA02629H10.1039/D0TA02629H ↗
26. Takehisa F. · 2018 · 301
27. 10.1016/0022-3697(65)90140-X10.1016/0022-3697(65)90140-X ↗
28. 10.1038/s41699-019-0116-410.1038/s41699-019-0116-4 ↗
29. 10.1016/j.jallcom.2019.03.26810.1016/j.jallcom.2019.03.268 ↗
30. 10.1103/PhysRevLett.108.16660110.1103/PhysRevLett.108.166601 ↗
31. 10.1021/acs.jpcc.7b0751110.1021/acs.jpcc.7b07511 ↗
32. 10.1038/ncomms921110.1038/ncomms9211 ↗
33. 10.1021/acsami.0c1781010.1021/acsami.0c17810 ↗
34. 10.1016/S0169-4332(98)00252-910.1016/S0169-4332(98)00252-9 ↗
35. 10.1016/S0169-4332(99)00265-210.1016/S0169-4332(99)00265-2 ↗