2017
DOI: 10.1364/oe.25.013626
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Short and broadband silicon asymmetric Y-junction two-mode (de)multiplexer using fast quasiadiabatic dynamics

Abstract: A short and broadband silicon asymmetric Y-junction two-mode (de)multiplexer is proposed and simulated. An adiabaticity parameter suitable for high index-contrast silicon waveguides is defined. The fast quasiadiabatic dynamics protocol is used to homogeneously distribute adiabaticity over the device length. This protocol limits the power coupled into the unwanted waveguide eigenmode under a fixed value along the propagation. A 16 μm long mode (de)multiplexer with crosstalk < -34 dB is obtained. Simulations sho… Show more

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Cited by 59 publications
(28 citation statements)
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“…Previously, the FAQUAD strategy was applied to homogenize the adiabaticity in mode (de)multiplexing Y-junctions where the two modes have the same polarization [29,30]. From the analysis above, we have successfully verified that the FAQUAD strategy can be applied to the analysis of eigenmodes which goes through polarization conversion via mode hybridization, showing the versatility of the FAQUAD approach.…”
Section: The Faquad Strategymentioning
confidence: 67%
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“…Previously, the FAQUAD strategy was applied to homogenize the adiabaticity in mode (de)multiplexing Y-junctions where the two modes have the same polarization [29,30]. From the analysis above, we have successfully verified that the FAQUAD strategy can be applied to the analysis of eigenmodes which goes through polarization conversion via mode hybridization, showing the versatility of the FAQUAD approach.…”
Section: The Faquad Strategymentioning
confidence: 67%
“…The result in Eq. 8improves the previous FAQUAD algorithm in [29,30], where the adiabaticity parameter and z are not completely decoupled in the analysis, leading to a less than optimal FAQUAD design. We use a commercial software (FIMMWAVE, Photon Design) [34] employing a finite difference method (FDM) to calculate the transverse component of the electric field E 2t and magnetic field H 3t associated with the second eigenmode (TM 0 to TE 1 ) and the third eigenmode (TE 1 to TM 0 ) of the taper, and the propagation constants β 2 of the second mode and β 3 of the third mode of the linear taper, and substitute E 2t , H 3t , β 2 and β 3 of the linear taper into Eq.…”
Section: The Faquad Strategymentioning
confidence: 89%
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