2019
DOI: 10.1002/andp.201800258
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Theoretical Design of a Pump‐Free Ultrahigh Efficiency All‐Optical Switching Based on a Defect Ring Optical Waveguide Network

Abstract: A theoretical design of a defect ring optical waveguide network is proposed to construct a pump-free ultrahigh efficiency all-optical switch. This switch creates ultrastrong photonic localization and causes the nonlinear dielectric in the defect waveguide to intensely respond. At its ON state, this material defect without Kerr response helps to produce a pair of sharp pass bands in the transmission spectrum to form the dual channel of the all-optical switch. When it is switched to its OFF state, the strong Ker… Show more

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Cited by 16 publications
(9 citation statements)
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“…At n0=1.63, the threshold control powers of the channels are EA16.4×1026 J, EA26.55×1026 J, EB13.54×1026 J, and EB23.81×1026 J, respectively. The EThre is significantly reduced, and it is five orders of magnitude larger than the previously reported result …”
Section: Optimizationcontrasting
confidence: 79%
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“…At n0=1.63, the threshold control powers of the channels are EA16.4×1026 J, EA26.55×1026 J, EB13.54×1026 J, and EB23.81×1026 J, respectively. The EThre is significantly reduced, and it is five orders of magnitude larger than the previously reported result …”
Section: Optimizationcontrasting
confidence: 79%
“…Our previous research introduced the defect nonlinear materials into a 1D periodic ring OWNs, and an excellent switching performance was obtained. This study attempts to optimize the all‐optical switching from three aspects: 1) using Model A from our previous research where the segment of nonlinear material defect is retained, but the length ratio of the waveguide segments is also increased; the rate of the first to the third cell of the waveguide length matching is d2:d1=3:1, and the rate of the length to the upper and lower arms of the intermediate cell is d3:d1=2.99:1, and shown as Figure a; 2) using Model B, which is based on Model A, but the number of defect segments of a nonlinear material is increased from one to two, as shown in Figure b; and 3) using both Models A and B and analyzing the difference between the refractive index of the linear and nonlinear material; the refractive index of the linear material, denoted as n1, is from 1.0 to 8.0 and the refractive index of the nonlinear material, denoted as n0, is from 1.45 to 1.63 . To make it convenient for experiment, the working wavelength is set to the communication wavelength λwork=1.55 μm.…”
Section: Models and Theoretical Methodsmentioning
confidence: 99%
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