Laser radar by taking liquid crystal device as light beam deflection device
A technology of liquid crystal devices and beam deflection, which is applied in instruments, optics, nonlinear optics, etc., can solve the problems of low diffraction efficiency and achieve low cost, good stability, and high reliability
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Embodiment 1
[0028] The first deflection unit includes a first liquid crystal phase retarder 1 and a first polarization grating 2, the first liquid crystal phase retarder is used to delay the incident light, and its phase retardation is a quarter wave plate, To convert the incident linearly polarized light into circularly polarized light or maintain linearly polarized light, the first polarization grating can deflect the incident light by an angle θ, where θ is greater than or equal to zero.
[0029] Thus, the first liquid crystal phase retarder 1 acts as a quarter-wave plate, which can convert linearly polarized light into circularly polarized light, and does not change the polarization state of the light when a high voltage is applied. The polarization grating 2 can realize the following functions: when the incident light is linearly polarized, the angle and polarization state of the light will not be changed; When the grating is used, the left-handed circularly polarized light and the r...
Embodiment 2
[0031] There are multiple second deflection units, and the multiple second deflection units are arranged in a row, and each deflection unit deflects or does not deflect the angle of light.
[0032] Thus, the total retardation of one or two or more liquid crystal phase retarders 1 reaches the effect of a half-wave plate, which can convert left (right) circularly polarized light into right (left) circularly polarized light, or one of them can add When the voltage is high, the circular (linear) polarized light can be converted into linear (circular) polarized light, or the polarization state of the light can not be changed when the voltage is applied at the same time. The combination of i systems can realize angular deflection from 0° to i*θ (i=1, 2, 3 . . . ).
Embodiment 3
[0034] A second deflection system 60 is included, the second deflection system 60 is located at the rear end of the first deflection system 50, and the second deflection system 60 is used to adjust the deflected light of the first deflection system 50 to a maximum deflection angle.
[0035] Thus, the second deflection system 60 can deflect the incident light by 2*i*θ (θ is the deflection angle of a single deflection grating, i=0,1,2... depends on the number of subsystems Bi ). If the polarization state of light before the second deflection system 60 is circularly polarized light, when the liquid crystal device in B1 works at high voltage, the polarization state of the light does not change after passing through the liquid crystal device, and it is still circularly polarized light. After the grating, the light is deflected by 2*θ. If the liquid crystal devices with m subsystems in the second deflection system work under high voltage (without changing the polarization state of ...
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