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1. S. A. Maier, Plasmonics: fundamentals and applications, 1st ed. (Springer, New York, 2007).
2. W. Jiang, B. Y. S. Kim, J. T. Rutka, and W. C. W. Chan, “Nanoparticle-mediated cellular response is size-dependent,” Nat. Nanotechnol. 3, 145 (2008).
3. P. K. Jain, K. S. Lee, I. H. El-Sayed, and M. A. El-Sayed, “Calculated absorption and scattering properties of gold nanoparticles of different size, shape, and composition: Applications in biological imaging and biomedicine,” J. Phys. Chem. B 110, 7238 (2006).
4. B. Luk'yanchuk, N. I. Zheludev, S. A. Maier, N. J. Halas, P. Nordlander, H. Giessen, and C. T. Chong, “The Fano resonance in plasmonic nanostructures and metamaterials,” Nat. Mater. 9, 707 (2010).
5. M. Rahmani, B. Luk'yanchuk, and M. H. Hong, “Fano resonance in novel plasmonic nanostructures,” Laser Photon. Rev. 7, 329 (2013).
6. S. Zhang, D. A. Genov, Y. Wang, M. Liu, and X. Zhang, “Plasmon-induced transparency in metamaterials,” Phys. Rev. Lett. 101, 047401 (2008).
7. F. Hao, Y. Sonnefraud, P. V. Dorpe, S. A. Maier, N. J. Halas, and P. Nordlander, “Symmetry breaking in plasmonic nanocavities: Subradiant LSPR sensing and a tunable Fano resonance,” Nano Lett. 8, 3983 (2008).
8. W. Cao, R. Singh, I. A. I. Al-Naib, M. X. He, A. J. Taylor, and W. L. Zhang, “Low-loss ultra-high-Q dark mode plasmonic Fano metamaterials,” Opt. Lett. 37, 3366 (2012).
9. D. DeJarnette, P. Blake, G. T. Forcherio, and D. K. Roper, “Far-field Fano resonance in nanoring lattices modeled from extracted, point dipole polarizability,” J. Appl. Phys. 115, 024306 (2014).
10. V. Dillu and R. K. Sinha, “Enhanced Fano resonance in silver ellipsoidal plasmonic crystal cavity,” J. Appl. Phys. 114, 234305 (2013).
11. Z. K. Zhou, X. N. Peng, Z. J. Yang, Z. S. Zhang, M. Li, X. R. Su, Q. Zhang, X. Shan, Q. Q. Wang, and Z. Zhang, “Tuning Gold Nanorod-Nanoparticle Hybrids into Plasmonic Fano Resonance for Dramatically Enhanced Light Emission and Transmission,” Nano Lett. 11, 49 (2010).
12. H. Chen, L. Shao, T. Ming, K. C. Woo, Y. C. Man, J. Wang, and H. Q. Lin, “Observation of the Fano resonance in gold nanorods supported on high-dielectric-constant substrates,” ACS Nano 5, 6754 (2011).
13. S. Zhang, K. Bao, N. J. Halas, H. Xu, and P. Nordlander, “Substrate-induced Fano resonances of a plasmonic nanocube: A route to increased-sensitivity localized surface plasmon resonance sensors revealed,” Nano Lett. 11, 1657 (2011).
14. H. Liu, X. Wu, B. Li, C. Xu, G. Zhang, and L. Zheng, “Fano resonance in two-intersecting nanorings: Multiple layers of plasmon hybridizations,” Appl. Phys. Lett. 100, 153114 (2012).
15. H. Lu, X. M. Liu, D. Mao, and G. X. Wang, “Plasmonic nanosensor based on Fano resonance in waveguide-coupled resonators,” Opt. Lett. 37, 3780 (2012).
16. F. Hao, P. Nordlander, Y. Sonnefraud, P. V. Dorpe, and S. A. Maier, “Tunability of subradiant dipolar and Fano-type plasmon resonances in metallic ring/disk cavities: Implications for nanoscale optical sensing,” ACS Nano 3, 643 (2009).
17. Y. F. Xiao, X. F. Jiang, Q. F. Yang, L. Wang, K. Shi, Y. Li and Q. Gong, “Tunneling-induced transparency in a chaotic microcavity,” Laser Photonics Rev. 7, L51 (2013).
18. P. Alonso-González, M. Schnell, P. Sarriugarte, H. Sobhani, C. Wu, N. Arju, A. Khanikaev, F. Golmar, P. Albella, L. Arzubiaga, F. Casanova, L. E. Hueso, P. Nordlander, G. Shvets, and R. Hillenbrand, “Real-space mapping of Fano interference in plasmonic metamolecules,” Nano Lett. 11, 3922 (2011).
19. J. Chen, Q. Shen, Z. Chen, Q. Wang, C. Tang, and Z. Wang, “Multiple Fano resonances in monolayer hexagonal non-close-packedmetallic shells,” J. Chem. Phys. 136, 214703 (2012).
20. D. Dregely, M. Hentschel, and H. Giessen, “Excitation and tuning of higher-order Fano resonances in plasmonic oligomer clusters,” ACS Nano 5, 8202 (2011).
21. Y. Cui, J. Zhou, V. A. Tamma, and W. Park, “Dynamic tuning and symmetry lowering of Fano resonance in plasmonic nanostructure,” ACS Nano 6, 2385 (2012).
22. S. D. Liu, Z. Yang, R. P. Liu, and X. Y. Li, “Multiple Fano resonances in plasmonic heptamer clusters composed of split nanorings,” ACS Nano 6, 6260 (2012).
23. S. D. Liu, Y. B. Yang, Z. H. Chen, W. J. Wang, H. M. Fei, M. J. Zhang, and Y. C. Wang, “Excitation of multiple Fano resonances in plasmonic clusters with D2h point group symmetry,” J. Phys. Chem. C 117, 14218 (2013).
24. Y. Wang, Z. Li, K. Zhao, A. Sobhani, X. Zhu, Z. Fang, and N. J. Halas, “Substrate-mediated charge transfer plasmons in simple and complex nanoparticle clusters,” Nanoscale 5, 9897 (2013).
25. Z. J. Yang, Q. Q. Wang, and H. Q. Lin, “Tunable two types of Fano resonances in metal–dielectric core–shell nanoparticle clusters,” Appl. Phys. Lett. 103, 111115 (2013).
26. J. Zhang and A. Zayats, “Multiple Fano resonances in single-layer nonconcentric core-shell nanostructures,” Opt. Express 21, 8426 (2013).
27. J. Wang, C. Fan, J. He, P. Ding, E. Liang, and Q. Xue, “Double Fano resonances due to interplay of electric and magnetic plasmon modes in planar plasmonic structure with high sensing sensitivity,” Opt. Express 21, 2236 (2013).
28. Y. Zhang, T. Q. Jia, H. M. Zhang, and Z. Z. Xu, “Fano resonances in disk–ring plasmonic nanostructure: strong interaction between bright dipolar and dark multipolar mode,” Opt. Lett. 37, 4919 (2012).
29. A. D. Khan, S. D. Khan, R. U. Khan, and N. Ahmad, “Excitation of multiple Fano-like resonances induced by higher order plasmon modes in three-layered bimetallic nanoshell dimer,” Plasmonics 9, 461 (2014).
30. N. Verellen, Y. Sonnefraud, H. Sobhani, F. Hao, V. V. Moshchalkov, P. Van Dorpe, P. Nordlander, and S. A. Maier, “Fano Resonances in Individual Coherent Plasmonic Nanocavities,” Nano Lett. 9, 1663 (2009).
31. Y. H. Fu, J. B. Zhang, Y. F. Yu, and B. Luk′yanchuk, “Generating and manipulating higher order Fano resonances in dual-disk ring plasmonic nanostructures,” ACS Nano 6, 5130 (2012).
32. N. Liu, M. Hentschel, T. Weiss, A. P. Alivisatos, and H. Giessen, “Three-dimensional plasmon rulers,” Science 332, 1407 (2011).
33. A. Artar, A. A. Yanik, and H. Altug, “Directional double Fano resonances in plasmonic hetero-oligomers,” Nano Lett. 11, 3694 (2011).
34. N. Liu, S. Mukherjee, K. Bao, L. V. Brown, J. Dorfmüller, P. Nordlander, and N. J. Halas, “Magnetic plasmon formation and propagation in artificial aromatic molecules,” Nano Lett. 12, 364 (2012).
35. B. B. Li, Y. F. Xiao, C. L. Zou, Y. C. Liu, X. F. Jiang, Y. L. Chen, Y. Li, and Q. Gong, “Experimental observation of Fano resonance in a single whispering-gallery microresonator,” Appl. Phys. Lett. 98, 021116 (2011).
36. Y. Zhang, F. Wen, Y. R. Zhen, P. Nordlander, and N. J. Halas, “Coherent Fano resonances in a plasmonic nanocluster enhance optical four-wave mixing,” Proc. Natl. Acad. Sci. U. S. A. 110, 9215 (2013).
37. Q. Zhang, X. Wen, G. Li, Q. Ruan, J. Wang, and Q. Xiong, “Multiple magnetic mode-based Fano resonance in split-ring resonator/disk nanocavities,” ACS Nano 7, 11071 (2013).
38. J. H. Shi, Z. Zhu, H. F. Ma, W. X. Jiang, and T. J. Cui, “Tunable symmetric and asymmetric resonances in an asymmetrical split-ring metamaterial,” J. Appl. Phys. 112, 073522 (2012).
39. Z. J. Yang, Z. S. Zhang, L. H. Zhang, Q. Q. Li, Z. H. Hao, and Q. Q. Wang, “Fano resonances in dipole-quadrupole plasmon coupling nanorod dimers,” Opt. Lett. 36, 1542 (2011).
40. M. Abb, Y. Wang, P. Albella, C. H. de Groot, J. Aizpurua, and O. L. Muskens, “Interference, coupling, and nonlinear control of high-order modes in single asymmetric nanoantennas,” ACS Nano 6, 6462 (2012).
41. J. A. Fan, C. Wu, K. Bao, J. Bao, R. Bardhan, N. J. Halas, V. N. Manoharan, P. Nordlander, G. Shvets, and F. Capasso, “Self-assembled plasmonic nanoparticle clusters,” Science 328, 1135 (2010).
42. M. Hentschel, M. Saliba, R. Vogelgesang, H. Giessen, A. P. Alivisatos, and N. Liu, “Transition from isolated to collective modes in plasmonic oligomers,” Nano Lett. 10, 2721 (2010).
43. M. Rahmani, B. Luk'yanchuk, T. Tahmasebi, Y. Lin, T. Liew, and M. Hong, “Polarization-controlled spatial localization of near-field energy in planar symmetric coupled oligomers,” Appl. Phys. A: Mater. Sci. Process. 107, 23 (2012).
44. M. Rahmani, E. Yoxall, B. Hopkins, Y. Sonnefraud, Y. Kivshar, M. Hong, C. Phillips, S. A. Maier, and A. E. Miroshnichenko, “Plasmonic nanoclusters with rotational symmetry: polarization-invariant far-field response vs changing near-field distribution,” ACS Nano 7, 11138 (2013).
45. M. Rahmani, D. Y. Lei, V. Giannini, B. Luk'yanchuk, M. Ranjbar, T. Y. F. Liew, M. H. Hong, and S. A. Maier, “Subgroup Decomposition of Plasmonic Resonances in Hybrid Oligomers: Modeling the Resonance Lineshape,” Nano Lett. 12, 2101 (2012).
46. J. B. Lassiter, H. Sobhani, M. W. Knight, W. S. Mielczarek, P. Nordlander, and N. J. Halas, “Designing and Deconstructing the Fano Lineshape in Plasmonic Nanoclusters,” Nano Lett. 12, 1058 (2012).
47. M. Rahmani, B. Luk'yanchuk, T. T. V. Nguyen, T. Tahmasebi, Y. Lin, T. Y. F. Liew, and M. H. Hong, “Influence of symmetry breaking in pentamers on Fano resonance and near-field energy localization,” Opt. Mater. Express 1, 1409 (2011).
48. E. Prodan, C. Radloff, N. J. Halas, and P. Nordlander, “A hybridization model for the plasmon response of complex nanostructures,” Science 302, 419 (2003).
49. J. Li, Y. Zhang, T. Jia, and Z. Sun, “High tunability multipolar Fano resonances in dual-ring/disk cavities,” Plasmonics (2014).
50. A. Taflove, and S. C. Hagness, Computational Electrodynamics: The Finite-Difference Time-Domain Method (Artech House, Boston, 2005).
51. P. B. Johnson and R. W. Christy, “Optical constants of the noble metals,” Phys. Rev. B 6, 4370 (1972).
52. H. Chen, L. Shao, T. Ming, K. C. Woo, Y. C. Man, J. Wang, and H. Q. Lin, “Observation of the Fano resonance in gold nanorods supported on high-dielectric-constant substrates,” ACS Nano 5, 6754 (2011).
53. F. Hao, P. Nordlander, M. T. Burnett, and S. A. Maier, “Enhanced tunability and linewidth sharpening of plasmon resonances in hybridized metallic ring/disk nanocavities,” Phys. Rev. B 76, 245417 (2007).
54. K. S. Lee and M. A. El-Sayed, “Dependence of the enhanced optical scattering efficiency relative to that of absorption for gold metal nanorods on aspect ratio, size, end-cap shape, and medium refractive index,” J. Phys. Chem. B 109, 20331 (2005).
55. J. Zuloaga and P. Nordlander, “On the energy shift between near-field and far-field peak intensities in localized plasmon systems,” Nano Lett. 11, 1280 (2011).
56. P. Alonso-González, P. Albella, F. Neubrech, C. Huck, J. Chen, F. Golmar, F. Casanova, L. E. Hueso, A. Pucci, J. Aizpurua, and R. Hillenbrand, “Experimental verification of the spectral shift between near- and far-field peak intensities of plasmonic infrared nanoantennas,” Phys. Rev. Lett. 110, 203902 (2013).
57. J. Chen, P. Albella, Z. Pirzadeh, P. Alonso-González, F. Huth, S. Bonetti, V. Bonanni, J. Akerman, J. Nogués, P. Vavassori, A. Dmitriev, J. Aizpurua, and R. Hillenbrand, “Plasmonic nickel nanoantennas,” Small 7, 2341 (2011).
58. P. Muhlschlegel, H. J. Eisler, O. J. F. Martin, B. Hecht, and D. W. Pohl, “Resonant optical antennas,” Science 308, 1607 (2005).

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Dark mode which is subradiant plays a key role in the generation of Fano effect. This study proposes that plasmon interaction between dark modes is a favorable method to generate multiple Fano resonances, where plasmon hybridization leads to the formation of a subradiant bonding and a subradiant antibonding combination. It demonstrates that a concentric ring/ring cavity dimer introduces interactions that render bonding quadrupolar ring mode dipole active, resulting in a pronounced Fano resonance. The corresponding antibonding quadrupolar ring mode is excited in a symmetry breaking nonconcentric cavity dimer, and double Fano resonances appear in the spectra.


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