Two-dimensional independently and continuously adjusted all-optical path control method and device
A technology of a control device and a control method, which is applied in the field of optics, can solve the problems that cannot be adjusted independently, and the conditions for realizing all-optical optical path control are harsh, and achieve the effect of convenient and continuous adjustment
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Embodiment 1
[0020] The two-dimensional independently and continuously adjustable all-optical optical path control method of the present invention comprises the following steps:
[0021] Step 1, generating a bundle of fundamental mode Gaussian beams and a bundle of (0,1) mode Laguerre Gaussian beams with the same polarization, same frequency, and same transmission direction;
[0022] Step 2, making the generated fundamental mode Gaussian beam and (0,1) mode Laguerre Gaussian beam concentrically and coherently superimposed on the incident surface of the nonlinear medium;
[0023] Step 3, by adjusting the ratio coefficient b and the phase difference δ of the two beams, respectively adjust the magnitude and direction of the center of gravity of the composite beam in the nonlinear medium from the initial position, thereby realizing two-dimensional independently and continuously adjustable plenoptic optical path control.
[0024] Its physical basis is the two-dimensional independent continuous ...
Embodiment 2
[0039] like figure 1 As shown, a two-dimensional independently and continuously adjustable plenoptic optical path control device includes a laser light source 1, a beam splitter 2, b beam splitter 11, a reflector 6, b reflector 5, and a vortex phase plate 3 , phase retarder 4, a attenuator 8, b attenuator 7, a beam reducer 10, b beam reducer 9, nonlinear body medium 12, wherein:
[0040] The initial fundamental mode Gaussian beam 13 emitted by the laser light source 1 is divided into two beams by the a beam splitter 2, one of which remains unchanged and is still the fundamental mode Gaussian beam 15, and the other beam passes through the vortex phase plate 3 and becomes into a (0,1) modulo Laguerre-Gaussian beam14.
[0041] Fundamental mode Gaussian beam 15 sequentially passes through phase retarder 4, a mirror 6, a attenuation plate 8 and then enters a beam reducer 10, (0,1) mode Laguerre Gaussian beam 14 sequentially passes through b mirror 5, b attenuation After the sheet...
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