Properties of Photonic and Plasmonic Resonance Devices Jae Woong Yoon, Kyu Jin Lee, Manoj Niraula, Mohammad Shyiq Amin, and Robert Magnusson Dept. of Electrical.

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Presentation transcript:

Properties of Photonic and Plasmonic Resonance Devices Jae Woong Yoon, Kyu Jin Lee, Manoj Niraula, Mohammad Shyiq Amin, and Robert Magnusson Dept. of Electrical Engineering, University of Texas – Arlington, TX 76019, United States

Outline Introduction Guided-mode resonance bandpass filters. Broadband omnidirectional Si grating absorbers. Transmission resonances in metallic nanoslit arrays. Gain-assisted ultrahigh-Q SPR in metallic nanocavity arrays. Conclusion 2

Photonic Resonances in Periodic Thin Films 3 Thin-film interference Guided mode by TIR Guided-mode resonance - Highly controllable with the pattern’s geometry. - Spectral engineering by blending of multiple guided modes.

Guided-Mode Resonances in Dielectric and Semiconductor Thin-Film Gratings Low index-contrast gratingsHigh index-contrast gratings - High-Q, narrow band resonances. - Primarily reflection peaks. - Optical notch filters, biosensors, and so on. - Both broadband + narrow-band effects. - Versatile spectral engineering. - Lossless mirrors/polarizers, flat microlenses, bandpass filters, broadband resonant absorbers, and so on. [Wang and Magnusson, Appl. Opt. 32, 2606 (1993)] [Ding and Magnusson, Opt. Express 12, 5661 (2004)] 4

Bandpass Filters: Theoretical Multilayer GMR Conventional multilayer Single-layer GMR structure Major advantages - Simple fab. processes (involves less fabrication errors). - Stop-bands and pass-line are determined by geometry of the surface texture. 5

Surface profiles (AFM) DesignFabricated Performance Parameters - Pass-line (peak): 0.4 nm FWHM, 83% efficiency. - Stop-band: < 1% over 100 nm bandwidth. - Angular tunability = 6 nm/deg. Bandpass Filters: Experimental 6

Broadband Omnidirectional Absorbers: Theoretical 340 nm  -Si:H SiO 2 30 nm 2000 nm 15.5% fill factor  = 419 nm Planar absorber GMR absorber 7

Broadband Omnidirectional Absorbers: Theoretical Anti-Reflection EffectResonant Light Trapping 8

Broadband Omnidirectional Absorbers: Experiment 9

Surface Plasmon Resonances in Metallic Nanostructures 10 Collective oscillation of surface free electrons. Deep subwavelength confinement: - Metallic metamaterials. - Optical communication with nanoscopic objects. - Quantum optical effects. Highly lossy due to ohmic damping. Primarily absorption and transmission resonances. (↔ Photonic resonances)

Extraordinary Optical Transmission Nature ; Phys. Rev. B SPP Destructively interfere 11

Extraordinary Optical Transmission Destructively interfere CM Fabry-Perot resonance of slit guided mode SPP resonance condition Cao et al., Phys. Rev. Lett (2002) “Negative role of surface plasmons in the transmission of metallic gratings with very narrow slits” 12

Surface and Cavity Plasmonic Resonances in Metallic Nanoslit Arrays 13

Toward Ultrahigh-Q Metallic Nanocavity Resonances 14

Conclusion Demonstrated optical bandpass filters and broadband absorbers based on high-index contrast subwavelength waveguide gratings. Explained complex resonance effects in metallic nanoslit arrays with a simple model of an optical cavity with Fano- resonant reflection boundaries. The theory predicts efficient room-T ultrahigh-Q plasmonic nanocavity resonances with the externally amplified intracavity feedback mechanism. 15

ACKNOWLEDGEMENT This research was supported, in part, by the UT System Texas Nanoelectronics Research Superiority Award funded by the State of Texas Emerging Technology Fund as well as by the Texas Instruments distinguished University Chair in Nanoelectronics endowment. Additional support was provided by the National Science Foundation (NSF) under Award No. ECCS and IIP Publications with these works: [1] J. W. Yoon, K. J. Lee, W. Wu, and R. Magnusson, “Wideband omnidirectional polarization- insensitive light absorbers made with 1D silicon gratings”, Adv. Opt. Mater. 2014; doi: /adom [2] J. W. Yoon, J. H. Lee, S. H. Song, and R. Magnusson, “Unified theory of surafce-plasmonic enhancement and extinction of light transmission through metallic nanoslit arrays”, Sci. Rep. 4, 5683 (2014). [3] J. W. Yoon, S. H. Song, and R. Magnusson, “Ultrahigh-Q metallic nanocavity resonances with externally-amplified intracavity feedback”, Sci. Rep. 4, 7124 (2014).