2017
DOI: 10.1109/lpt.2016.2624747
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Polarization-Independent Modulator by Partly Tilted Graphene-Induced Electro-Absorption Effect

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Cited by 28 publications
(13 citation statements)
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“…Although the polarization-independent electro-optic modulator based on graphene has been reported [ 15 21 ], the polarization independence of these devices is closely related to wavelength [ 22 ]. Therefore, in our model, the U-structure is used, in which we find that the sensitivity of the waveguide polarization is weak correlation with wavelength.…”
Section: Resultsmentioning
confidence: 99%
“…Although the polarization-independent electro-optic modulator based on graphene has been reported [ 15 21 ], the polarization independence of these devices is closely related to wavelength [ 22 ]. Therefore, in our model, the U-structure is used, in which we find that the sensitivity of the waveguide polarization is weak correlation with wavelength.…”
Section: Resultsmentioning
confidence: 99%
“…Besides the above-analyzed optical properties of the proposed hybrid graphene-silicon-based polarization-insensitive EAM, its corresponding electrical characteristics are also critical, such as the 3 dB modulation bandwidth ( f 3dB ) and the energy consumption ( E ), which are associated with the total capacitance ( C ) and resistance ( R ) of the optical device, f 3dB = 1/(2 πRC ), E = CV 2 /4 ( V stands for the switching voltage between “OFF” and “ON” states) [ 40 , 42 ]. Here, we estimated the electrical characteristics of the proposed EAM using the parallel plate capacitor and the equivalent electrical circuit model for simplicity [ 27 , 28 , 29 ]. By considering the multilayer hybrid graphene-silicon waveguide structure and the overlapping region between graphene layers, the total resistance of the device is estimated to be ~80 Ω (including the graphene sheet resistance and the metal-graphene contact resistance) and the total capacitance ( C ) is estimated to be ~326 fF.…”
Section: Resultsmentioning
confidence: 99%
“…Meanwhile, hexagonal boron nitride (hBN) was used as the spacer or insulating layer to encapsulate graphene layers and maintain the high carrier mobility of graphene [30]. By optimizing the dimensions of all hybrid graphene-silicon waveguide layers, polarization-insensitive modulation was realized with an ME of ~1.11 dB/µm and an ME discrepancy of lower than 0.006 dB/µm for both polarizations, which are better than previous reports [28,29]. We then propose a hybrid graphene-silicon-based polarization-insensitive EAM with a modulation length of 20 µm.…”
Section: Introductionmentioning
confidence: 99%
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“…The two graphene layers, which are separated by a 10 nm thick Si 3 N 4 spacer, are also surrounded by an outer waveguide with the width and height of 800 nm and 800 nm. For fabrication, it is better to replacing the rectangular silicon-graphene waveguide with a slanted silicon-graphene waveguide for the inner waveguide [22]. Metal electrodes are in contact with the graphene layers, so that the two graphene layers can form capacitor structures.…”
Section: Polarization-insensitive Waveguide Structurementioning
confidence: 99%