64 research outputs found

    Purcell effect in Hyperbolic Metamaterial Resonators

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    The radiation dynamics of optical emitters can be manipulated by properly designed material structures providing high local density of photonic states, a phenomenon often referred to as the Purcell effect. Plasmonic nanorod metamaterials with hyperbolic dispersion of electromagnetic modes are believed to deliver a significant Purcell enhancement with both broadband and non-resonant nature. Here, we have investigated finite-size cavities formed by nanorod metamaterials and shown that the main mechanism of the Purcell effect in these hyperbolic resonators originates from the cavity hyperbolic modes, which in a microscopic description stem from the interacting cylindrical surface plasmon modes of the finite number of nanorods forming the cavity. It is found that emitters polarized perpendicular to the nanorods exhibit strong decay rate enhancement, which is predominantly influenced by the rod length. We demonstrate that this enhancement originates from Fabry-Perot modes of the metamaterial cavity. The Purcell factors, delivered by those cavity modes, reach several hundred, which is 4-5 times larger than those emerging at the epsilon near zero transition frequencies. The effect of enhancement is less pronounced for dipoles, polarized along the rods. Furthermore, it was shown that the Purcell factor delivered by Fabry-Perot modes follows the dimension parameters of the array, while the decay rate in the epsilon near-zero regime is almost insensitive to geometry. The presented analysis shows a possibility to engineer emitter properties in the structured metamaterials, addressing their microscopic structure

    Purcell effect in Hyperbolic Metamaterial Resonators

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    The radiation dynamics of optical emitters can be manipulated by properly designed material structures providing high local density of photonic states, a phenomenon often referred to as the Purcell effect. Plasmonic nanorod metamaterials with hyperbolic dispersion of electromagnetic modes are believed to deliver a significant Purcell enhancement with both broadband and non-resonant nature. Here, we have investigated finite-size cavities formed by nanorod metamaterials and shown that the main mechanism of the Purcell effect in these hyperbolic resonators originates from the cavity hyperbolic modes, which in a microscopic description stem from the interacting cylindrical surface plasmon modes of the finite number of nanorods forming the cavity. It is found that emitters polarized perpendicular to the nanorods exhibit strong decay rate enhancement, which is predominantly influenced by the rod length. We demonstrate that this enhancement originates from Fabry-Perot modes of the metamaterial cavity. The Purcell factors, delivered by those cavity modes, reach several hundred, which is 4-5 times larger than those emerging at the epsilon near zero transition frequencies. The effect of enhancement is less pronounced for dipoles, polarized along the rods. Furthermore, it was shown that the Purcell factor delivered by Fabry-Perot modes follows the dimension parameters of the array, while the decay rate in the epsilon near-zero regime is almost insensitive to geometry. The presented analysis shows a possibility to engineer emitter properties in the structured metamaterials, addressing their microscopic structure

    Near-Field Interference for the Unidirectional Excitation of Electromagnetic Guided Modes

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    Wave interference is a fundamental manifestation of the superposition principle with numerous applications. Although in conventional optics, interference occurs between waves undergoing different phase advances during propagation, we show that the vectorial structure of the near field of an emitter is essential for controlling its radiation as it interferes with itself on interaction with a mediating object. We demonstrate that the near-field interference of a circularly polarized dipole results in the unidirectional excitation of guided electromagnetic modes in the near field, with no preferred far-field radiation direction. By mimicking the dipole with a single illuminated slit in a gold film, we measured unidirectional surface-plasmon excitation in a spatially symmetric structure. The surface wave direction is switchable with the polarization.This work has been supported in part by the Engineering and Physical Sciences Research Council (grant EP/H000917/2). F.J.R.-F. acknowledges support from grant FPI of Generalitat Valenciana. A. M. acknowledges financial support from the Spanish government (contracts Consolider EMET CSD2008-00066 and TEC2011-28664-C02-02). P. G. acknowledges the Royal Society for a Newton International Fellowship.Rodríguez Fortuño, FJ.; Marino, G.; Ginzburg, P.; O’connor, D.; Martínez Abietar, AJ.; Wurtz, GA.; Zayats, AV. (2013). Near-Field Interference for the Unidirectional Excitation of Electromagnetic Guided Modes. Science. 340(6130):328-330. https://doi.org/10.1126/science.1233739S3283303406130Yu, N., Genevet, P., Kats, M. A., Aieta, F., Tetienne, J.-P., Capasso, F., & Gaburro, Z. (2011). Light Propagation with Phase Discontinuities: Generalized Laws of Reflection and Refraction. Science, 334(6054), 333-337. doi:10.1126/science.1210713Ni, X., Emani, N. K., Kildishev, A. V., Boltasseva, A., & Shalaev, V. M. (2011). Broadband Light Bending with Plasmonic Nanoantennas. Science, 335(6067), 427-427. doi:10.1126/science.1214686Merlin, R. (2007). Radiationless Electromagnetic Interference: Evanescent-Field Lenses and Perfect Focusing. Science, 317(5840), 927-929. doi:10.1126/science.1143884Pendry, J. B. (2000). Negative Refraction Makes a Perfect Lens. Physical Review Letters, 85(18), 3966-3969. doi:10.1103/physrevlett.85.3966Helseth, L. E. (2008). The almost perfect lens and focusing of evanescent waves. Optics Communications, 281(8), 1981-1985. doi:10.1016/j.optcom.2007.12.018Eleftheriades, G. V., & Wong, A. M. H. (2008). Holography-Inspired Screens for Sub-Wavelength Focusing in the Near Field. IEEE Microwave and Wireless Components Letters, 18(4), 236-238. doi:10.1109/lmwc.2008.918871Lee, J. Y., Hong, B. H., Kim, W. Y., Min, S. K., Kim, Y., Jouravlev, M. V., … Kim, K. S. (2009). Near-field focusing and magnification through self-assembled nanoscale spherical lenses. Nature, 460(7254), 498-501. doi:10.1038/nature08173Stockman, M. I., Faleev, S. V., & Bergman, D. J. (2002). Coherent Control of Femtosecond Energy Localization in Nanosystems. Physical Review Letters, 88(6). doi:10.1103/physrevlett.88.067402Aeschlimann, M., Bauer, M., Bayer, D., Brixner, T., Cunovic, S., Fischer, A., … Voronine, D. V. (2012). Optimal open-loop near-field control of plasmonic nanostructures. New Journal of Physics, 14(3), 033030. doi:10.1088/1367-2630/14/3/033030Sukharev, M., & Seideman, T. (2006). Phase and Polarization Control as a Route to Plasmonic Nanodevices. Nano Letters, 6(4), 715-719. doi:10.1021/nl0524896Barnes, W. L., Dereux, A., & Ebbesen, T. W. (2003). Surface plasmon subwavelength optics. Nature, 424(6950), 824-830. doi:10.1038/nature01937Schuller, J. A., Barnard, E. S., Cai, W., Jun, Y. C., White, J. S., & Brongersma, M. L. (2010). Plasmonics for extreme light concentration and manipulation. Nature Materials, 9(3), 193-204. doi:10.1038/nmat2630Kim, H., & Lee, B. (2009). Unidirectional Surface Plasmon Polariton Excitation on Single Slit with Oblique Backside Illumination. Plasmonics, 4(2), 153-159. doi:10.1007/s11468-009-9086-2Bonod, N., Popov, E., Li, L., & Chernov, B. (2007). Unidirectional excitation of surface plasmons by slanted gratings. Optics Express, 15(18), 11427. doi:10.1364/oe.15.011427Bouillard, J.-S., Vilain, S., Dickson, W., Wurtz, G. A., & Zayats, A. V. (2012). Broadband and broadangle SPP antennas based on plasmonic crystals with linear chirp. Scientific Reports, 2(1). doi:10.1038/srep00829Li, X., Tan, Q., Bai, B., & Jin, G. (2011). Experimental demonstration of tunable directional excitation of surface plasmon polaritons with a subwavelength metallic double slit. Applied Physics Letters, 98(25), 251109. doi:10.1063/1.3602322Radko, I. P., Bozhevolnyi, S. I., Brucoli, G., Martin-Moreno, L., Garcia-Vidal, F. J., & Boltasseva, A. (2009). Efficient unidirectional ridge excitation of surface plasmons. Optics Express, 17(9), 7228. doi:10.1364/oe.17.007228Liu, Y., Palomba, S., Park, Y., Zentgraf, T., Yin, X., & Zhang, X. (2012). Compact Magnetic Antennas for Directional Excitation of Surface Plasmons. Nano Letters, 12(9), 4853-4858. doi:10.1021/nl302339zCurto, A. G., Volpe, G., Taminiau, T. H., Kreuzer, M. P., Quidant, R., & van Hulst, N. F. (2010). Unidirectional Emission of a Quantum Dot Coupled to a Nanoantenna. Science, 329(5994), 930-933. doi:10.1126/science.1191922Laroche, M., Arnold, C., Marquier, F., Carminati, R., Greffet, J.-J., Collin, S., … Pelouard, J.-L. (2005). Highly directional radiation generated by a tungsten thermal source. Optics Letters, 30(19), 2623. doi:10.1364/ol.30.002623Roelkens, G., Vermeulen, D., Van Laere, F., Selvaraja, S., Scheerlinck, S., Taillaert, D., … Baets, R. (2010). Bridging the Gap Between Nanophotonic Waveguide Circuits and Single Mode Optical Fibers Using Diffractive Grating Structures. Journal of Nanoscience and Nanotechnology, 10(3), 1551-1562. doi:10.1166/jnn.2010.2031Hansen, W. N. (1968). Electric Fields Produced by the Propagation of Plane Coherent Electromagnetic Radiation in a Stratified Medium. Journal of the Optical Society of America, 58(3), 380. doi:10.1364/josa.58.000380Rotenberg, N., Spasenović, M., Krijger, T. L., le Feber, B., García de Abajo, F. J., & Kuipers, L. (2012). Plasmon Scattering from Single Subwavelength Holes. Physical Review Letters, 108(12). doi:10.1103/physrevlett.108.127402Ruan, Z., & Fan, S. (2010). Superscattering of Light from Subwavelength Nanostructures. Physical Review Letters, 105(1). doi:10.1103/physrevlett.105.01390

    Active Inference, Novelty and Neglect

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    In this chapter, we provide an overview of the principles of active inference. We illustrate how different forms of short-term memory are expressed formally (mathematically) through appealing to beliefs about the causes of our sensations and about the actions we pursue. This is used to motivate an approach to active vision that depends upon inferences about the causes of 'what I have seen' and learning about 'what I would see if I were to look there'. The former could manifest as persistent 'delay-period' activity - of the sort associated with working memory, while the latter is better suited to changes in synaptic efficacy - of the sort that underlies short-term learning and adaptation. We review formulations of these ideas in terms of active inference, their role in directing visual exploration and the consequences - for active vision - of their failures. To illustrate the latter, we draw upon some of our recent work on the computational anatomy of visual neglect

    Superluminal and stopped light due to mode coupling in confined hyperbolic metamaterial waveguides

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    Anisotropic metamaterials with hyperbolic dispersion can be used to design waveguides with unusual properties. We show that, in contrast to planar waveguides, geometric confinement leads to coupling of ordinary (forward) and extraordinary (backward) modes and formation of hybrid waveguided modes, which near the crossing point may exhibit slow, stopped or superluminal behavior accompanied by very strong group velocity dispersion. These modes can be used for designing stopped-light nanolasers for nanophotonic applications and dispersion-facilitated signal reshaping in telecom applications

    Ultrafast hybrid plasmonics

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    Anisotropic plasmonic metamaterials for nanophotonic applications

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