M-Point Lasing in Hexagonal and Honeycomb Plasmonic Lattices
Source abstract
Abstract
This paper reports the observation of band-edge states at the high-symmetry M-point in the first Brillouin zone of hexagonal and honeycomb plasmonic nanoparticle (NP) lattices. The surface lattice resonance at the M-point (SLRM) of a hexagonal lattice results from asymmetric out-of-plane dipole coupling between NPs. In contrast to the hexagonal lattice, honeycomb lattices support two SLR modes at the M-point because of their non-Bravais nature: (1) a blue-shifted SLRM1 from the coupling of two distinct out-of-plane dipole LSP resonances, and (2) a red-shifted SLRM2 from in-plane dipole–dipole coupling. By incorporating organic dye solutions as gain media with Ag NP lattices, we achieved M-point lasing from both hexagonal and honeycomb lattices. Understanding coupling mechanisms at high-symmetry points in NP lattices with the same geometry but different unit cells is important to assess the prospects of topological states in plasmonic systems.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Plasmonic and Surface Plasmon Research · Photonic Crystals and Applications · Strong Light-Matter Interactions
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Materials Science and Engineering, Northwestern University, Evanston, Illinois 60208, United States
Department of Chemistry, Northwestern University, Evanston, Illinois 60208, United States
Center for Nanoscale Materials, Argonne National Laboratory, Lemont, Illinois 60439, United States
Funding
U.S. Department of Defense · Division of Materials Research
References (42)
Show source-provided references
1. 10.1364/JOSAB.10.00028310.1364/JOSAB.10.000283 ↗
2. 10.1103/PhysRevE.58.389610.1103/PhysRevE.58.3896 ↗
3. 10.1364/AO.55.00B13910.1364/AO.55.00B139 ↗
4. 10.1103/PhysRevLett.92.12390610.1103/PhysRevLett.92.123906 ↗
5. 10.1063/1.290821210.1063/1.2908212 ↗
6. 10.1038/nmeth71410.1038/nmeth714 ↗
7. 10.1038/nmat350310.1038/nmat3503 ↗
8. 10.1021/jp026731y10.1021/jp026731y ↗
9. Maier, S. A. Plasmonics: Fundamentals and Applications; Springer: New York, NY, 2007; Vol. 1, p 224.10.1007/0-387-37825-1 ↗
10. 10.1038/nnano.2013.9910.1038/nnano.2013.99 ↗
11. 10.1038/nnano.2017.12610.1038/nnano.2017.126 ↗
12. 10.1364/JOSAB.36.00E10410.1364/JOSAB.36.00E104 ↗
13. 10.1073/pnas.200881811710.1073/pnas.2008818117 ↗
14. 10.1021/acsnano.9b0114210.1021/acsnano.9b01142 ↗
15. 10.1103/PhysRevB.95.15542310.1103/PhysRevB.95.155423 ↗
16. 10.1021/acsnano.9b0946610.1021/acsnano.9b09466 ↗
17. 10.1021/acs.nanolett.9b0534210.1021/acs.nanolett.9b05342 ↗
18. 10.1073/pnas.161528111310.1073/pnas.1615281113 ↗
19. 10.1021/acs.nanolett.9b0266110.1021/acs.nanolett.9b02661 ↗
20. 10.1039/D0NA00095G10.1039/D0NA00095G ↗
21. 10.1021/acsnano.0c0479510.1021/acsnano.0c04795 ↗
22. 10.1021/acs.nanolett.8b0177410.1021/acs.nanolett.8b01774 ↗
23. 10.1103/PhysRevLett.122.01390110.1103/PhysRevLett.122.013901 ↗
24. 10.1103/PhysRevB.90.07540410.1103/PhysRevB.90.075404 ↗
25. 10.1002/lpor.20140046210.1002/lpor.201400462 ↗
26. 10.1002/adom.20160076810.1002/adom.201600768 ↗
27. 10.1002/adom.20140051310.1002/adom.201400513 ↗
28. 10.1103/PhysRevB.96.04541710.1103/PhysRevB.96.045417 ↗
29. 10.1088/1367-2630/18/10/10302910.1088/1367-2630/18/10/103029 ↗
30. 10.1103/PhysRevB.97.14420310.1103/PhysRevB.97.144203 ↗
31. 10.1021/acs.nanolett.9b0481310.1021/acs.nanolett.9b04813 ↗
32. 10.1021/ph400094910.1021/ph4000949 ↗
33. 10.1103/PhysRevLett.114.22390110.1103/PhysRevLett.114.223901 ↗
34. 10.1126/science.aaq032710.1126/science.aaq0327 ↗
35. 10.1515/nanoph-2019-040810.1515/nanoph-2019-0408 ↗
36. 10.1021/acs.nanolett.1c0184110.1021/acs.nanolett.1c01841 ↗
37. 10.1021/nl102206x10.1021/nl102206x ↗
38. 10.1021/ar050013n10.1021/ar050013n ↗
39. 10.1038/nnano.2007.25210.1038/nnano.2007.252 ↗
40. 10.1021/acs.jpclett.9b0107610.1021/acs.jpclett.9b01076 ↗
41. 10.1021/acsphotonics.0c0023110.1021/acsphotonics.0c00231 ↗
42. Palik E. D. · 1991 · 2