Topology Optimization of High‐Performance Optomechanical Resonator
Source abstract
Abstract
Abstract High quality mechanical resonators are critical for driving advances in quantum information technologies, precision sensing, and optomechanics. However, achieving compact resonator designs that maintain high performance is a key challenge. In this study, a new class of compact resonators optimized to operate at higher‐order eigenmodes is presented, achieving both high frequencies and enhanced quality factor‐frequency ( Qf ) products. By employing topology optimization to maximize the damping dilution factor, these resonators achieve minimized edge bending losses and enhanced intrinsic damping. Their high‐( Qf ) performance and compact form factor position these resonators as promising candidates for applications in quantum information transduction, advanced optomechanical systems, and next‐generation sensing technologies.
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Research context
OpenAlex topics: Mechanical and Optical Resonators · Force Microscopy Techniques and Applications · Advanced Thermodynamic Systems and Engines
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Center for Macroscopic Quantum States (bigQ) Department of Physics Technical University of Denmark Fysikvej Kgs. Lyngby 2800 Denmark
Department of Civil and Mechanical Engineering Technical University of Denmark Koppel's Allé 404 Kgs. Lyngby 2800 Denmark
Funding
Novo Nordisk Fonden · Danmarks Grundforskningsfond · Villum Fonden
References (42)
Show source-provided references
1. 10.1103/PhysRevApplied.15.L02100110.1103/PhysRevApplied.15.L021001 ↗
2. Pratt J. R. · Phys. Rev. X · 2023 · 13
3. 10.1103/PhysRevApplied.14.01404210.1103/PhysRevApplied.14.014042 ↗
4. 10.1038/s41586-022-04720-210.1038/s41586-022-04720-2 ↗
5. 10.1007/978-3-319-28691-410.1007/978-3-319-28691-4 ↗
6. Engelsen N. J. · Nat. Nanotechnol. · 2024 · 1
7. 10.1063/1.114869210.1063/1.1148692 ↗
8. 10.1063/1.220482910.1063/1.2204829 ↗
9. 10.1016/S0375-9601(00)00411-410.1016/S0375-9601(00)00411-4 ↗
10. 10.1038/nnano.2017.10110.1038/nnano.2017.101 ↗
11. 10.1126/science.aar693910.1126/science.aar6939 ↗
12. 10.1038/s41467-024-48183-710.1038/s41467-024-48183-7 ↗
13. Høj D. · Phys. Rev. X · 2024 · 14
14. 10.1103/PhysRevLett.124.02550210.1103/PhysRevLett.124.025502 ↗
15. 10.1038/s41467-022-30586-z10.1038/s41467-022-30586-z ↗
16. Bereyhi M. J. · Phys. Rev. X · 2022 · 12
17. 10.1021/acs.nanolett.8b0494210.1021/acs.nanolett.8b04942 ↗
18. 10.1103/PhysRevLett.116.14720210.1103/PhysRevLett.116.147202 ↗
19. 10.1002/adma.20210624810.1002/adma.202106248 ↗
20. Bendsoe M. P. · 2013
21. 10.1016/j.cma.2019.11269210.1016/j.cma.2019.112692 ↗
22. 10.1038/s41467-021-26102-410.1038/s41467-021-26102-4 ↗
23. Bathe K.‐J. · 2006
24. Cook R. D. · 2007
25. 10.1103/RevModPhys.86.139110.1103/RevModPhys.86.1391 ↗
26. 10.1103/PhysRevLett.113.22720110.1103/PhysRevLett.113.227201 ↗
27. 10.1016/j.aop.2013.08.00310.1016/j.aop.2013.08.003 ↗
28. Wb tot: total bending energy evaluated with targeted normalized eigenmode profile in COMSOL using shell.Ws_tot with the global evaluation feature.Wb clamp: bending energy of domain near clamping boundaries spanning 10μm$\umu\rm{m}$ evaluated in COMSOL using shell. WsA with the surface integral feature.
29. 10.1103/PhysRevApplied.15.L02100110.1103/PhysRevApplied.15.L021001 ↗
30. Reinhardt C. · Phys. Rev. X · 2016 · 6
31. Pratt J. R. · Phys. Rev. X · 2023 · 13
32. 10.1108/eb02356210.1108/eb023562 ↗
33. 10.1007/s00419-007-0142-010.1007/s00419-007-0142-0 ↗
34. 10.1007/BF0165094910.1007/BF01650949 ↗
35. 10.1007/s00158-010-0602-y10.1007/s00158-010-0602-y ↗
36. 10.1007/s00158010012910.1007/s001580100129 ↗
37. 10.1016/j.cma.2015.05.00310.1016/j.cma.2015.05.003 ↗
38. 10.1007/s00158-015-1265-510.1007/s00158-015-1265-5 ↗
39. 10.1016/S0045-7949(99)00056-510.1016/S0045-7949(99)00056-5 ↗
40. 10.1002/nme.162024020710.1002/nme.1620240207 ↗
41. 10.1080/17415979408802757310.1080/174159794088027573 ↗
42. 10.1007/s00158-006-0087-x10.1007/s00158-006-0087-x ↗