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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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( 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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( 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: