Device and method for moving self-focusing point of round Airy beam in large-range and high-precision manner
A self-focusing, large-scale technology, applied in optics, optical components, nonlinear optics, etc., can solve the problem of inconvenient application of circular Airy beam optical tweezers, and achieve the effect of simple device and avoiding inaccuracy
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Embodiment 1
[0035] Such as figure 1 As shown, the present invention provides a device for moving the self-focusing point of a circular Airy beam with high precision in a large range, including a laser, a polarizer, a first lens, a second lens, a spatial light modulator, a plane mirror, and a third lens and charge couplers;
[0036] The laser outputs fundamental mode Gaussian light. After being polarized by the polarizer, the beam is expanded by the 4f system composed of the first lens and the second lens, so that when it enters the spatial light modulator, it fills up the liquid crystal screen. On the spatial light modulator Load the spectral information of the circular Airy beam, and control the two-dimensional plane of the self-focus point of the circular Airy beam by shifting the spectrum; after being modulated by the spatial light modulator and reflected by the plane mirror, it passes through the third lens Fourier After leaf transformation, a circular Airy beam is obtained at the fo...
Embodiment 2
[0041] Such as figure 1 , As shown in 2 and 3, the present invention also provides a method for moving the self-focus point of a circular Airy beam with high precision in a large range, including the following steps:
[0042] The fundamental-mode Gaussian beam output by the laser (Verdi 12 solid-state laser, working wavelength 532nm) is polarized by the polarizer, and then expanded by plano-convex lenses placed parallel and vertically. The spatial light modulator (1920 × 1080 resolution) developed by Relike Information Co., Ltd. is used to load the expanded Gaussian beam on the expanded Gaussian beam, which contains the spectral information after the translation of the circular Airy beam and the kinoform of the blazed grating (such as figure 2 As shown in (b), after the Fourier transform of the lens, because of the addition of the blazed grating phase, it is necessary to use a diaphragm to filter out one level, and a circular Airy beam can be seen at its focal plane, and a ci...
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