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2d finite difference time domain (fdtd) solver  (Optiwave Systems Inc)

 
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    Optiwave Systems Inc 2d finite difference time domain (fdtd) solver
    ( a ) 3D schematic of the nano-antenna using Si (red) and the SWG-engineered metamaterial (blue). ( b ) The far-field radiation pattern of the nano-antenna at a wavelength of 1550 nm. ( c ) 3D <t>FDTD</t> simulation of the nano-antenna radiated power (left axis) and peak radiation angle (right axis) as a function of the wavelength.
    2d Finite Difference Time Domain (Fdtd) Solver, supplied by Optiwave Systems Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/product/2d+finite+difference+time+domain+(fdtd)+solver/2d+finite+difference+time+domain++fdtd++solver/pmc09182638-54-9-17
    Average 90 stars, based on 1 article reviews
    2d finite difference time domain (fdtd) solver - by Bioz Stars, 2026-09
    90/100 stars

    Images

    1) Product Images from "Circular Optical Phased Arrays with Radial Nano-Antennas"

    Article Title: Circular Optical Phased Arrays with Radial Nano-Antennas

    Journal: Nanomaterials

    doi: 10.3390/nano12111938

    ( a ) 3D schematic of the nano-antenna using Si (red) and the SWG-engineered metamaterial (blue). ( b ) The far-field radiation pattern of the nano-antenna at a wavelength of 1550 nm. ( c ) 3D FDTD simulation of the nano-antenna radiated power (left axis) and peak radiation angle (right axis) as a function of the wavelength.
    Figure Legend Snippet: ( a ) 3D schematic of the nano-antenna using Si (red) and the SWG-engineered metamaterial (blue). ( b ) The far-field radiation pattern of the nano-antenna at a wavelength of 1550 nm. ( c ) 3D FDTD simulation of the nano-antenna radiated power (left axis) and peak radiation angle (right axis) as a function of the wavelength.

    Techniques Used:

    Related Articles

    other:

    Article Title: Circular Optical Phased Arrays with Radial Nano-Antennas
    Article Snippet: Grating coupler simulations were performed by using a commercial 2D finite difference time domain (FDTD) solver by Optiwave to optimize its structural and performance parameters.



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    ( a ) 3D schematic of the nano-antenna using Si (red) and the SWG-engineered metamaterial (blue). ( b ) The far-field radiation pattern of the nano-antenna at a wavelength of 1550 nm. ( c ) 3D <t>FDTD</t> simulation of the nano-antenna radiated power (left axis) and peak radiation angle (right axis) as a function of the wavelength.
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    ( a ) 3D schematic of the nano-antenna using Si (red) and the SWG-engineered metamaterial (blue). ( b ) The far-field radiation pattern of the nano-antenna at a wavelength of 1550 nm. ( c ) 3D <t>FDTD</t> simulation of the nano-antenna radiated power (left axis) and peak radiation angle (right axis) as a function of the wavelength.
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    Image Search Results


    ( a ) 3D schematic of the nano-antenna using Si (red) and the SWG-engineered metamaterial (blue). ( b ) The far-field radiation pattern of the nano-antenna at a wavelength of 1550 nm. ( c ) 3D FDTD simulation of the nano-antenna radiated power (left axis) and peak radiation angle (right axis) as a function of the wavelength.

    Journal: Nanomaterials

    Article Title: Circular Optical Phased Arrays with Radial Nano-Antennas

    doi: 10.3390/nano12111938

    Figure Lengend Snippet: ( a ) 3D schematic of the nano-antenna using Si (red) and the SWG-engineered metamaterial (blue). ( b ) The far-field radiation pattern of the nano-antenna at a wavelength of 1550 nm. ( c ) 3D FDTD simulation of the nano-antenna radiated power (left axis) and peak radiation angle (right axis) as a function of the wavelength.

    Article Snippet: Grating coupler simulations were performed by using a commercial 2D finite difference time domain (FDTD) solver by Optiwave to optimize its structural and performance parameters.

    Techniques: