Four-wave mixing holographic multiplexing method based on nonlinear metasurface
A four-wave mixing, nonlinear technology, applied in the field of micro-nano holography
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Embodiment 1
[0050] Such as figure 1As shown, in the four-wave mixing holographic multiplexing method based on the nonlinear metasurface disclosed in this embodiment, the metasurface for realizing nonlinear space and frequency multiplexing is composed of an array of gold nano-rectangular hole structures with different geometric sizes. By changing the geometric size of the gold nano-rectangular hole structure, the nonlinear metasurface can arbitrarily regulate the amplitude and phase of the outgoing nonlinear frequency signal. The complex amplitude distribution of the outgoing nonlinear optical field under different sizes is obtained by full-wave vector calculation. The amplitude type hologram is calculated based on the optimized GS algorithm, and the gold rectangular hole structure is encoded to the hologram according to the bit coding method. The GS algorithm is an optimization algorithm s that iterates on the holographic surface and the reconstruction surface during the hologram calcula...
Embodiment 1
[0068] The four-wave mixing holographic multiplexing method based on the nonlinear metasurface disclosed in the first embodiment utilizes the four-wave mixing effect of gold nanometer rectangular holes to realize space and frequency multiplexing of amplitude holography. Adjusting λ by changing the length and width of the gold nano-rectangular hole FWM1 and at λ FWM2 The complex amplitude of the corresponding outgoing nonlinear light field component at ; find the satisfying in λ FWM1 and at λ FWM2The amplitude at the place satisfies two-bit encoding, and the four gold nanometer rectangular hole structures with uniform phases are used for holographic multiplexing encoding. Two holograms carrying independent information are obtained by calculation and the selected gold nano-rectangular pore structure is encoded on the same metasurface. By selecting the outgoing component parallel to the incident light field, it is achieved at λ FWM1 produces a reconstructed image 'A' at λ FW...
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