Environmental Temperature's Impact on Ultrafast Photoacoustic Conversion in 2D Layered Semiconductor/3D Dielectric Heterostructure
Source abstract
Abstract
Abstract For a 2D layered semiconductor/3D dielectric heterostructure, longitudinal coherent acoustic phonon (CAP) oscillation of 2D layers can emit a picosecond acoustic (PA) pulse into 3D materials. However, the environmental temperature's impact on the ultrafast photoacoustic conversion across the van der Waals heterointerface remains elusive. Here, employing femtosecond laser pump‐probe, the dynamical correlation between CAP oscillations and emitted PA pulses are experimentally investigated in a MoS 2 /SiO 2 heterostructure when varying the environmental temperature from 294 to 364 K. It turns out that interlayer expansion of MoS 2 layers leads to a redshift of CAP oscillation frequency. Meanwhile, enhanced phonon scatterings both in MoS 2 layers and at the MoS 2 /SiO 2 heterointerface collectively reduce ultrafast photoacoustic energy conversion efficiency. The results provide insights for understanding heat‐mediated ultrafast photoacoustic conversions in a 2D layered semiconductor heterostructure.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: 2D Materials and Applications · Ga2O3 and related materials · Perovskite Materials and Applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
State Key Laboratory of Digital Medical Engineering, School of Biological Science and Medical Engineering Southeast University Nanjing 210096 China
School of Physics Southeast University Nanjing 210096 China
School of Electronic Science and Engineering Southeast University Nanjing 210096 China
Funding
National Key Research and Development Program of China · Natural Science Foundation of Jiangsu Province · National Natural Science Foundation of China
References (36)
Show source-provided references
1. 10.3390/cryst1104035510.3390/cryst11040355 ↗
2. 10.1038/s41467-021-23359-710.1038/s41467-021-23359-7 ↗
3. 10.1103/PhysRevLett.105.13680510.1103/PhysRevLett.105.136805 ↗
4. 10.1103/PhysRevB.90.20542210.1103/PhysRevB.90.205422 ↗
5. 10.1557/jmr.2015.32410.1557/jmr.2015.324 ↗
6. 10.1039/C5CS00507H10.1039/C5CS00507H ↗
7. 10.1021/acs.nanolett.3c0231610.1021/acs.nanolett.3c02316 ↗
8. 10.1063/1.192986910.1063/1.1929869 ↗
9. 10.1021/acs.nanolett.2c0000310.1021/acs.nanolett.2c00003 ↗
10. 10.1103/PhysRevB.98.07540810.1103/PhysRevB.98.075408 ↗
11. 10.1016/j.pacs.2023.10048910.1016/j.pacs.2023.100489 ↗
12. 10.1016/j.pacs.2023.10050910.1016/j.pacs.2023.100509 ↗
13. 10.1364/PRJ.7.00141610.1364/PRJ.7.001416 ↗
14. 10.1063/1.477252810.1063/1.4772528 ↗
15. 10.1038/s41563-021-00922-710.1038/s41563-021-00922-7 ↗
16. 10.1016/j.ultras.2014.06.00510.1016/j.ultras.2014.06.005 ↗
17. 10.1103/PhysRevB.70.12520810.1103/PhysRevB.70.125208 ↗
18. 10.1103/PhysRevB.108.06431010.1103/PhysRevB.108.064310 ↗
19. 10.1103/PhysRevB.34.412910.1103/PhysRevB.34.4129 ↗
20. 10.1021/nl404297r10.1021/nl404297r ↗
21. 10.1103/PhysRevB.87.11541310.1103/PhysRevB.87.115413 ↗
22. 10.1038/srep0572210.1038/srep05722 ↗
23. 10.1364/PRJ.49180510.1364/PRJ.491805 ↗
24. 10.1063/1.499313210.1063/1.4993132 ↗
25. 10.1063/1.346745910.1063/1.3467459 ↗
26. 10.1021/acs.nanolett.2c0134410.1021/acs.nanolett.2c01344 ↗
27. 10.1364/PRJ.44211410.1364/PRJ.442114 ↗
28. 10.1021/acsnano.6b0225310.1021/acsnano.6b02253 ↗
29. 10.1039/C4NR04602A10.1039/C4NR04602A ↗
30. 10.1016/0022-3697(76)90143-810.1016/0022-3697(76)90143-8 ↗
31. 10.1021/nl304169w10.1021/nl304169w ↗
32. 10.1021/acsnano.7b0270310.1021/acsnano.7b02703 ↗
33. 10.3390/nano1012254310.3390/nano10122543 ↗
34. 10.1103/PhysRevB.103.02430210.1103/PhysRevB.103.024302 ↗
35. 10.1103/PhysRevB.93.07542010.1103/PhysRevB.93.075420 ↗
36. 10.7498/aps.73.2023164810.7498/aps.73.20231648 ↗