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• W2023696568 abstract "The Si <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>3</sub> N <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>4</sub> waveguide offers very low propagation loss and feasibility for three-dimensional photonic integration, but it suffers from large optical mode size (thus low integration density) due to the relatively small refractive index contrast between the Si <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>3</sub> N <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>4</sub> core and the SiO <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>2</sub> cladding. On the other hand, the metal-insulator-metal plasmonic waveguide offers very tight light confinement but it suffers from large propagation loss. In this work, we integrate Cu-Si <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>3</sub> N <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>4</sub> -Cu nanoplasmonic waveguides along with various passive components with the conventional Si <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>3</sub> N <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>4</sub> waveguides. The Cu-Si <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>3</sub> N <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>4</sub> -Cu waveguide exhibits ~0.37-dB/μm propagation loss at telecommunication wavelengths of 1550 nm and ~45% coupling efficiency with the conventional 1-μm-wide S <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>3</sub> N <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>4</sub> waveguide through a simple 2-μm-long tapered coupler. Ultracompact 1×2 and 1×4 plasmonic power splitters can split light almost equally with an excess loss of ~3.5 dB and ~1 dB, respectively." @default.
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• W2023696568 date "2012-12-01" @default.
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• W2023696568 title "Experimental demonstration of integrated horizontal Cu-Si<inf>3</inf>N<inf>4</inf>-Cu plasmonic waveguide and passive components" @default.
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• W2023696568 doi "https://doi.org/10.1109/pgc.2012.6457949" @default.
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