Journal
NATURE MATERIALS
Volume 9, Issue 9, Pages 707-715Publisher
NATURE PUBLISHING GROUP
DOI: 10.1038/NMAT2810
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Funding
- Agency for Science, Technology and Research (A*STAR) [082 141 0039, 102 152 0018]
- UK Engineering and Physical Sciences Research Council
- Royal Society
- US Department of Defense NSSEFF
- Robert A. Welch Foundation [C-1220, C-1222]
- US Department of Energy
- Deutsche Forschungsgemeinschaft of the Federal Republic of Germany [FOR 557, FOR 730, SPP1391]
- Bundesministerium fur Bildung und Forschung
- EPSRC [EP/D063329/1, EP/G060363/1, EP/H000917/2, EP/H000917/1] Funding Source: UKRI
- Engineering and Physical Sciences Research Council [EP/H000917/1, EP/H000917/2, EP/G060363/1, EP/D063329/1] Funding Source: researchfish
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Since its discovery, the asymmetric Fano resonance has been a characteristic feature of interacting quantum systems. The shape of this resonance is distinctively different from that of conventional symmetric resonance curves. Recently, the Fano resonance has been found in plasmonic nanoparticles, photonic crystals, and electromagnetic metamaterials. The steep dispersion of the Fano resonance profile promises applications in sensors, lasing, switching, and nonlinear and slow-light devices.
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