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• W3188694557 abstract "All-optical graphene-based optical modulators have recently attracted much attention because of their ultrafast and broadband response characteristics (bandwidth larger than 100 GHz) in comparison with the previous graphene-based optical modulators, which are electrically tuned via the graphene Fermi level. Silicon photonics has some benefits such as low cost and high compatibility with CMOS design and manufacturing technology. On the other hand, graphene has a unique large nonlinear Kerr coefficient, which we calculate using graphene’s tight-binding model based on the semiconductor Bloch equations. Its real and imaginary parts are negative at the wavelength of 1.55 µm and <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline> <mml:mrow class=MJX-TeXAtom-ORD> <mml:msub> <mml:mi>E</mml:mi> <mml:mi>F</mml:mi> </mml:msub> </mml:mrow> <mml:mo>=</mml:mo> <mml:mn>0.1</mml:mn> <mml:mspace width=thickmathspace /> <mml:mrow class=MJX-TeXAtom-ORD> <mml:mrow class=MJX-TeXAtom-ORD> <mml:mi mathvariant=normal>e</mml:mi> <mml:mi mathvariant=normal>V</mml:mi> </mml:mrow> </mml:mrow> </mml:math> . To simultaneously use the benefits mentioned above, we present an all-optical, CMOS-compatible, and graphene-on-silicon slot (GOSS) waveguide extinction and phase modulator that consists of two different geometries. The first one consists of a one-stage GOSS waveguide with a single layer of graphene. To increase the light–graphene interaction and consequently enhance the modulation efficiency (ME), another stage of the GOSS waveguide is placed over the first one. This two-stage configuration is called a graphene-on-silicon double-slot (GOSDS) waveguide. The ME, insertion loss (IL), and modulation depth (MD) for a 12.5 µm GOSDS waveguide modulator with a double layer of graphene can reach 0.241 dB/µm, 1.31 dB, and 77%, respectively, at optical pump intensities about <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline> <mml:mn>9</mml:mn> <mml:mspace width=thickmathspace /> <mml:mrow class=MJX-TeXAtom-ORD> <mml:mrow class=MJX-TeXAtom-ORD> <mml:mi mathvariant=normal>M</mml:mi> <mml:mi mathvariant=normal>W</mml:mi> </mml:mrow> </mml:mrow> <mml:mspace width=thinmathspace /> <mml:mrow class=MJX-TeXAtom-ORD> <mml:msup> <mml:mrow class=MJX-TeXAtom-ORD> <mml:mrow class=MJX-TeXAtom-ORD> <mml:mi mathvariant=normal>c</mml:mi> <mml:mi mathvariant=normal>m</mml:mi> </mml:mrow> </mml:mrow> <mml:mrow class=MJX-TeXAtom-ORD> <mml:mo>−<!-- − --></mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> . Our design has a smaller waveguide length (17.6 times) than the previous all-optical graphene-on-silicon ribbon waveguide extinction modulator and high MD (about 2 times) in comparison with a graphene-clad microfiber all-optical extinction modulator. Compared with an all-optical Mach–Zehnder interferometer phase modulator, our design has short graphene coated waveguide length ( <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline> <mml:mo>≈<!-- ≈ --></mml:mo> <mml:mspace width=negativethinmathspace /> <mml:mn>0.1</mml:mn> </mml:math> times) and low local optical intensities ( <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline> <mml:mo>≈<!-- ≈ --></mml:mo> <mml:mspace width=negativethinmathspace /> <mml:mn>0.043</mml:mn> </mml:math> times) needed for <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline> <mml:mi>π<!-- π --></mml:mi> </mml:math> phase shift. This study may promote the design and realization of high-performance, wideband, compact, and all-optical control on a single chip with a reasonable contrast level." @default.
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• W3188694557 date "2021-09-03" @default.
• W3188694557 modified "2023-10-16" @default.
• W3188694557 title "All-optical graphene-on-silicon slot waveguide modulator based on graphene’s Kerr effect" @default.
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• W3188694557 doi "https://doi.org/10.1364/ao.427755" @default.
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