Slow light waveguide device of photonic crystal based on two-dimensional silicon
A photonic crystal and optical waveguide technology, applied in the optical field, can solve the problems of inability to form slow light effects, destroying structural symmetry, weakening slow light effects, etc., achieving simple and easy efficiency, good signal fidelity, and large slow light bandwidth. Effect
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Embodiment 1
[0033] Example 1: Construct a low-scattering photonic crystal slow light waveguide device for the purpose of obtaining a larger bandwidth, using 1THz as the working frequency, a=65μm, the long axis b starts from 0.4a, and the gradual change step size △b=0.002a , take e=0.5 to obtain a terahertz frequency-domain two-dimensional silicon-based hole-shaped longitudinal gradient line-defect photonic crystal slow light waveguide device constructed by a specific circular segment scattering element, and use the above-mentioned implementation to obtain the group refractive index n of the device g =31.4, in low dispersion (group refractive index variation range n g within ±10%), ultra-low dispersion (group refractive index variation range n g Within ±1%) and close to zero dispersion, the bandwidths of slow light are 2.334 μm, 0.945 μm, and 0.91 μm respectively. The slow light waveguide device obtains a large flat bandwidth, and the slow light effect is stable.
Embodiment 2
[0034] Example 2: Construct a low-scattering photonic crystal slow light waveguide device for the purpose of obtaining a higher group refractive index. Other conditions are the same as in Example 1. Take e=0.35 to obtain a terahertz frequency constructed by another specific circular bow-shaped scattering element. Domain two-dimensional silicon-based hole-shaped longitudinal gradient line defect photonic crystal slow light waveguide structure, using the above implementation scheme, the group refractive index n of the device is obtained g =95.0, in the three cases of low dispersion, ultra-low dispersion and near-zero dispersion, the bandwidths of slow light are 0.736 μm, 0.438 μm, and 0.20 μm, indicating that this kind of slow light waveguide device can not only obtain a lower group velocity, but also A large flat bandwidth can be obtained, and the slow light effect is very stable. In the case of ensuring low dispersion, the group velocity and the slow light bandwidth can be flex...
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