A two-dimensional independently continuously adjustable all-optical optical path control method and device thereof
A technology of a control device and a control method, which is applied in the optical field, can solve the problems of inability to separate and independently adjust, and the realization conditions of 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 independent and continuously adjustable all-optical optical path control method of the present invention comprises the following steps:
[0021] Step 1, generating a fundamental mode Gaussian beam and a (0,1) mode Laguerre Gaussian beam with the same polarization, the same frequency, and the same transmission direction;
[0022] In step 2, the generated fundamental mode Gaussian beam and the (0,1) mode Laguerre Gaussian beam are superimposed concentrically and coherently on the incident surface of the nonlinear medium;
[0023] Step 3: Adjust the magnitude and direction of the deviation of the center of gravity of the composite beam in the nonlinear medium from the initial position by adjusting the proportional coefficient b and the phase difference δ of the two beams, thereby realizing two-dimensional independent and continuously adjustable all-optical optical path control.
[0024] Its physical basis is the two-dimensional independently continuousl...
Embodiment 2
[0039] like figure 1 As shown in the figure, a two-dimensional independent and continuously adjustable all-optical 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 attenuation plate 8, b attenuation plate 7, a beam reducer 10, b beam reducer 9, non-linear volume medium 12, wherein:
[0040] The initial fundamental mode Gaussian beam 13 emitted by the laser light source 1 is divided into two beams by 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 then changes into two beams. into a (0,1) mode Laguerre Gaussian beam 14 .
[0041] The fundamental mode Gaussian beam 15 enters the a beam reducer 10 through the phase retarder 4, the a mirror 6, and the a attenuation plate 8 in turn, and the (0, 1) mode Laguerre Gaussian beam 14 is atten...
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