2019
DOI: 10.1063/1.5094523
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Ultrafast saturable absorption dynamics in hybrid graphene/Si3N4 waveguides

Abstract: We study the nonlinear optical properties of graphene integrated onto Si3N4 waveguides under picosecond and subpicosecond pulsed excitation at telecom wavelength. Saturable absorption of graphene under guided-mode excitation is measured, and the temporal effects related to the photoexcited carrier dynamics in graphene are highlighted. Thereafter, a model of photoexcited carriers in graphene is implemented into the nonlinear Schrödinger equation in order to simulate the pulse propagation across the hybrid graph… Show more

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Cited by 88 publications
(93 citation statements)
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“…nanowire, which reflects the power dependent loss due solely to the GO films. The ΔEIL decreased as the pulse energy was increased -a trend that is consistent with saturable absorption (SA) [50,51] (see Section 4 for detailed discussion). We also note that these changes were not permanent -the measured insertion loss recovered to those in Figures 3(a-i) and (a-ii) when the pulse energy was reduced, with the measured EIL in Figures 4(b-i) and (b-ii) being repeatable.…”
Section: Nonlinear Loss Measurementmentioning
confidence: 56%
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“…nanowire, which reflects the power dependent loss due solely to the GO films. The ΔEIL decreased as the pulse energy was increased -a trend that is consistent with saturable absorption (SA) [50,51] (see Section 4 for detailed discussion). We also note that these changes were not permanent -the measured insertion loss recovered to those in Figures 3(a-i) and (a-ii) when the pulse energy was reduced, with the measured EIL in Figures 4(b-i) and (b-ii) being repeatable.…”
Section: Nonlinear Loss Measurementmentioning
confidence: 56%
“…In our calculations, we neglected any potential spectral/temporal coupling effects that could induce interplay between SA and SPM. This was because the length of the hybrid SOI nanowires was much shorter than the dispersion length for the picosecond pulses used, and so the change in the pulse spectrum due to SPM did not have a significant effect on the temporal shape of the pulse [50]. According to our simulations, the maximum difference induced by SPM on ΔEIL is < 1%.…”
Section: Spm Spectral Broadeningmentioning
confidence: 77%
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“…The maximum difference between them is < 0.2%, reflecting that the influence of SPM on SA is negligible. This is mainly because the total length of the hybrid waveguides (3 mm) was much shorter than the dispersion length (> 1 m), and so any change in the pulse spectrum induced by SPM did not significantly affect the temporal pulse shape [79].…”
Section: Discussionmentioning
confidence: 99%
“…These results reveal the strong potential of integrating 2D layered GO films on SiN devices to improve the nonlinear optical performance. SiN waveguides with a cross section of 1.6 μm × 0.66 μm were fabricated via annealing-free and crack-free processes that are compatible with CMOS fabrication [52,53]. First, a SiN layer was deposited via low-pressure chemical vapor deposition (LPCVD) in two steps, with a 370nm-thick layer for each, so as to control strain and to prevent cracks.…”
Section: Introductionmentioning
confidence: 99%