Littérature scientifique sur le sujet « V-SHAPED NANOANTENNA »

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Articles de revues sur le sujet "V-SHAPED NANOANTENNA"

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Zhou, Fei, Ye Liu et Weiping Cai. « Plasmonic holographic imaging with V-shaped nanoantenna array ». Optics Express 21, no 4 (12 février 2013) : 4348. http://dx.doi.org/10.1364/oe.21.004348.

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Yu, Yang, Jinze Liu, Yidu Yu, Dayong Qiao, Yongqian Li et Rafael Salas-Montiel. « Broadband unidirectional transverse light scattering in a V-shaped silicon nanoantenna ». Optics Express 30, no 5 (23 février 2022) : 7918. http://dx.doi.org/10.1364/oe.450943.

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Huang, Feng, Hanning Yang, Siren Li, Xiangqian Jiang et Xiudong Sun. « Tunable Unidirectional Coupling of Surface Plasmon Polaritons Utilizing a V-Shaped Slot Nanoantenna Column ». Plasmonics 10, no 6 (17 juin 2015) : 1825–31. http://dx.doi.org/10.1007/s11468-015-9988-0.

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Tanaka, Yoshito Y., Tomoya Kimura et Tsutomu Shimura. « Unidirectional emission of phase-controlled second harmonic generation from a plasmonic nanoantenna ». Nanophotonics 10, no 18 (13 octobre 2021) : 4601–9. http://dx.doi.org/10.1515/nanoph-2021-0470.

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Abstract Shaping the emission pattern of second harmonic (SH) generation from plasmonic nanoparticles is important for practical applications in nonlinear nanophotonics but is rendered challenging by the complex second-order nonlinear-optical processes. Here, we theoretically and experimentally demonstrate that a pair of V- and Y-shaped gold nanoparticles directs the SH emission perpendicularly to an incident light direction. Owing to spatial overlap of two orthogonal plasmonic dipole modes at the fundamental and SH wavelengths of the individual particles, surface SH polarizations induced by the fundamental field is efficiently near-field coupled to the SH plasmon mode, resulting in dipolar SH emission from the individual particles. Moreover, the phase of this emission can be tuned simply by altering the part of the Y-particle shape, which changes the SH plasmon resonance while keeping the fundamental resonance. Our approach is a promising platform for engineering not only directional nonlinear nanoantennas but also nonlinear metamaterials.
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Lv, Jingwei, Debao Wang, Chao Liu, Jianxin Wang, Lin Yang, Wei Liu, Qiang Liu, Haiwei Mu et Paul K. Chu. « Theoretical Analysis of Hybrid Metal–Dielectric Nanoantennas with Plasmonic Fano Resonance for Optical Sensing ». Coatings 12, no 9 (26 août 2022) : 1248. http://dx.doi.org/10.3390/coatings12091248.

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A nanoantenna with Fano response is designed with plasmonic oligomers as a refractive index sensor to enhance surface-enhanced Raman scattering (SERS) in the visible light spectrum. The scattered radiation and field-enhanced interactions of the outer gallium phosphide (GaP) nanoring assembled with an inner heptamer of silver with Fano response are investigated systematically using the finite element method. The characteristics of Fano resonance are found to depend on the size, shape and nature of the materials in the hybrid nanoantenna. The confined electromagnetic field produces a single-point electromagnetic hotspot with up to 159.59 V/m. The sensitivity obtained from the wavelength shift and variation in the scattering cross-section (SCS) shows a maximum value of 550 nm/RIU. The results validate the design concept and demonstrate near-field enhancement, enabling the design of high-performance nanoantennas with enhanced optical sensing and SERS properties.
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Klein, Michael F. G., Herbert Hein, Peter-Jürgen Jakobs, Stefan Linden, Nina Meinzer, Martin Wegener, Volker Saile et Manfred Kohl. « Electron beam lithography of V-shaped silver nanoantennas ». Microelectronic Engineering 86, no 4-6 (avril 2009) : 1078–80. http://dx.doi.org/10.1016/j.mee.2008.12.023.

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H. Mahdi, Rasha, et Hussein A. Jawad. « Thermal response of skin diseased tissue treated by plasmonic nanoantenna ». International Journal of Electrical and Computer Engineering (IJECE) 10, no 3 (1 juin 2020) : 2969. http://dx.doi.org/10.11591/ijece.v10i3.pp2969-2977.

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The thermal distribution in the diseased tissue treated by different methods faces the problem of an uncontrollable defused heat. In the present article, we use a plasmonic bowtie nanoantenna working in the near infrared region to enhance the temperature confinement in the tissue. The Computer Simulation Technology Studio Suite package version 2019 was used to execute the design of both plasmonic nanoantenna and the tissue. Gold nanostructure and silicon carbide dioxide are the components the plasmonic nanoantenna in the bowtie shape. The results showed that the distance between the tumor tissue and the antenna is important to determine the intensity field where the maximum field is 5.9*107 V/m at a distance of 100 nm. The maximum specific absorption rate is 1.92*1011 W/kg at a similar distance which gives a higher temperature in the tissue of 580 Co. It is concluded that from the obtained results that the near infrared (1064 nm) resonance wavelength is recommended in the treatment of cancer cell by plasmonic bowtie nanoantenna because higher intensity field is generated. The closer distance to the nanoantenna gives higher temperature in the tissue while the temperature gradually decreases in the tissue till 400 nm where no valuable temperature was detected.
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Jiao Jiao, 焦. 蛟., 罗先刚 Luo Xiangang et 赵. 青. Zhao Qing. « Design and Preparation of Planar Lens Based on V-Shaped Nanoantennas ». Acta Optica Sinica 37, no 7 (2017) : 0724001. http://dx.doi.org/10.3788/aos201737.0724001.

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Liu Yang, 刘阳, 周海京 Zhou Haijing et 李瀚宇 Li Hanyu. « Numerical simulation on directional side scattering of V-shaped gold sphere-array nanoantennas ». High Power Laser and Particle Beams 26, no 7 (2014) : 73210. http://dx.doi.org/10.3788/hplpb20142607.73210.

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Rashidi, Arash, M. T. Chryssomallis et D. E. Anagnostou. « Tailorable optical scattering properties of V-shaped plasmonic nanoantennas : a computationally efficient and fast analysis ». Journal of the Optical Society of America A 31, no 10 (19 septembre 2014) : 2256. http://dx.doi.org/10.1364/josaa.31.002256.

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Thèses sur le sujet "V-SHAPED NANOANTENNA"

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KUMAR, SHANU. « DESIGN AND ANALYSIS OF V-SHAPED NANOANTENNA ». Thesis, 2018. http://dspace.dtu.ac.in:8080/jspui/handle/repository/16533.

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To convert the energy of free propagating radiation to localized energy and localized energy into free propagating radiation energy, we have always been reliant on radio wave and microwave antennas. But with the developments in physical optics, optical antennas are garnering attraction. Properties of metal nanostructures which behave as strongly coupled plasmas at optical frequencies forms the basis for the operation of optical antennas. Optical antennas can overcome the limitations of light-emitting devices, photovoltaics and spectroscopy by increasing the light-matter interaction. Televisions, cell-phones and other communication equipment which work on electromagnetic antennas, mostly use radio-wave or microwave ambit of the electromagnetic spectrum. Contrary to the electromagnetic fields, optical frequencies are controlled by re-directing the wave fronts of propagating radiation by means of lenses, mirrors, and diffractive elements. There are several current studies which have been undertaken to find ways of translating established radio wave and microwave antenna theories into the optical frequency regime and with few successes attained with the help pf nano-optics and plasmonics, optical antennas may soon be a thing of practical use. Once we are able to extend the concept of antennas into optical frequency regime, we can have major technological advancements ranging from enhanced absorption cross-sections and quantum yields in photovoltaics, releasing energy efficiently from nanoscale lightemitting devices, boosting the efficiency of photochemical or photophysical detectors, to improving spatial resolution in optical microscopy.
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Actes de conférences sur le sujet "V-SHAPED NANOANTENNA"

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Kumar, Shanu, Pooja Chauhan et Ajeet Kumar. « Design and Analysis of a Cross V-shaped Nanoantenna for Visible Region ». Dans Frontiers in Optics. Washington, D.C. : OSA, 2018. http://dx.doi.org/10.1364/fio.2018.jtu3a.68.

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