All-optical multi-wavelength conversing method and device based on photonic crystal
A technology of photonic crystals and conversion devices, which is applied in light demodulation, light guides, optics, etc., can solve problems such as the limitation of the application range of all-optical wavelength conversion bands, saturation of optical power density, and impact on conversion efficiency, and achieve high-efficiency multi-wavelength selection. frequency output, high flexibility and freedom, simple and compact effect
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Embodiment 1
[0033] Such as figure 1 As shown, the linear photonic crystal-based all-optical multi-wavelength conversion device of this embodiment includes a continuous light single-frequency pump laser (CW LD) 1, an ultrashort pulse laser (Pulsed LD) 2, and a linear photonic crystal multi-wavelength conversion system (PC MWCS) 3. Between the continuous light single-frequency pump laser 1 and the linear photonic crystal multi-wavelength conversion system 3, a 50×microscopic objective lens 4 and a 50×microscopic objective lens 5 are sequentially arranged along the direction of the optical path; the linear photonic crystal multi-wavelength conversion system Between the conversion system 3 and the ultrashort pulse laser 2, a 50×microscopic objective lens 6, a half-transparent mirror 8, and a 50×microscopic objective lens 7 are sequentially arranged along the optical path direction. The operating wavelength of the continuous light single-frequency pump laser 1 is λ=(1550±1)nm, the center wavel...
Embodiment 2
[0045] Such as image 3 As shown, the present embodiment is all the same as embodiment 1 except the following features.
[0046] The point defect 16 of the rear linear photonic crystal reflective cavity mirror of the linear photonic crystal multi-wavelength conversion system is formed by a square dielectric column of 0.42a×0.42a or 0.46a×0.46a instead of the original circular dielectric column at this position.
[0047] This embodiment realizes the frequency-selective output of multiple wavelengths, because at this time the side length of the point defect is reduced from 0.8a×0.8a to 0.42a×0.42a (the wavelength of the corresponding defect mode is λ 01 ) or 0.46a×0.46a (the corresponding defect mode wavelength is λ 02 ), such that the multimode of point defect modes (λ 01 and lambda 02 ) becomes a single-mode (λ 01 or lambda 02 ). When the ultrashort pulse laser is incident from the waveguide, only a single defect mode in the point defect 16 can be excited out (that is, λ...
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