All‐Around HfO2 Stressor for Tensile Strain in GeSn‐on‐Insulator Nanobeam Lasers
Source abstract
Abstract
Abstract Tensile strained GeSn alloys are considered a key enabler for the realization of complementary metal‐oxide‐semiconductor laser sources. However, the tensile strained GeSn lasers reported to date require complex fabrication processes for applying tensile strain in GeSn, preventing tensile GeSn lasers from becoming the mainstream technology for integrated photonics. Here, a unique strain engineering method is presented that can introduce a uniform tensile strain in GeSn lasers by harnessing a widely developed atomic layer deposition (ALD) process. 1D photonic crystal nanobeam lasers under homogenous tensile strain induced by an ALD HfO2 all‐around stressor layer show a single‐mode lasing peak with a ≈31 nm redshift and ≈2 times intensity increase. The lasing threshold of tensile strained GeSn lasers is ≈12% improved compared to the unstrained GeSn lasers. It is believed that the approach offers a new path toward the realization of practical group‐IV laser sources for photonic‐integrated circuits.
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Research context
OpenAlex topics: Photonic and Optical Devices · Advanced Fiber Optic Sensors · Mechanical and Optical Resonators
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
School of Electrical and Electronic Engineering Nanyang Technological University 50 Nanyang Avenue Singapore 639798 Singapore
School of Electronic and Electrical Engineering University of Leeds Leeds LS2 9JT UK
Department of Physics and KI for the NanoCentury Korea Advanced Institute of Science and Technology (KAIST) Daejeon 34141 Republic of Korea
Funding
National Research Foundation Singapore
References (32)
Show source-provided references
1. 10.1109/JSTQE.2006.88315110.1109/JSTQE.2006.883151 ↗
2. 10.1038/lsa.2015.13110.1038/lsa.2015.131 ↗
3. 10.1364/OL.35.00067910.1364/OL.35.000679 ↗
4. 10.1364/OE.20.01131610.1364/OE.20.011316 ↗
5. 10.1021/nl401042n10.1021/nl401042n ↗
6. 10.1038/nphoton.2013.6710.1038/nphoton.2013.67 ↗
7. 10.1364/OE.23.01481510.1364/OE.23.014815 ↗
8. 10.1021/acs.nanolett.5b0397610.1021/acs.nanolett.5b03976 ↗
9. 10.1038/s41467-017-02026-w10.1038/s41467-017-02026-w ↗
10. 10.1063/1.502570510.1063/1.5025705 ↗
11. 10.1038/s41467-019-10655-610.1038/s41467-019-10655-6 ↗
12. 10.1063/1.365863210.1063/1.3658632 ↗
13. 10.1063/1.510887810.1063/1.5108878 ↗
14. 10.1063/5.004351110.1063/5.0043511 ↗
15. 10.1021/acsphotonics.9b0071210.1021/acsphotonics.9b00712 ↗
16. 10.1038/s41566-020-0601-510.1038/s41566-020-0601-5 ↗
17. 10.1038/nphoton.2013.19110.1038/nphoton.2013.191 ↗
18. 10.1002/adma.20120369210.1002/adma.201203692 ↗
19. 10.1103/PhysRevLett.118.07610110.1103/PhysRevLett.118.076101 ↗
20. 10.1038/s41563-019-0418-010.1038/s41563-019-0418-0 ↗
21. 10.1021/cr900056b10.1021/cr900056b ↗
22. 10.1016/j.mattod.2014.04.02610.1016/j.mattod.2014.04.026 ↗
23. 10.1021/acsnano.5b0524910.1021/acsnano.5b05249 ↗
24. 10.1364/OE.42632110.1364/OE.426321 ↗
25. 10.1063/5.006693510.1063/5.0066935 ↗
26. 10.1063/5.008747710.1063/5.0087477 ↗
27. 10.1364/PRJ.45544310.1364/PRJ.455443 ↗
28. 10.1002/advs.20220761110.1002/advs.202207611 ↗
29. 10.1063/1.494365210.1063/1.4943652 ↗
30. 10.1002/advs.20220761110.1002/advs.202207611 ↗
31. 10.1109/LED.2016.260316210.1109/LED.2016.2603162 ↗
32. 10.1002/adom.20210121310.1002/adom.202101213 ↗