Vector Beam Amplification and Generation Device with Polarization-Independent Optical Parametric Amplification
A technology of optical parametric amplification and polarization, which is applied in the field of optoelectronics, can solve the problems that the vector beam is difficult to amplify and the vector beam is difficult to generate, and achieves the effect of simple production process
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Embodiment 1
[0045] Set the wavelength of the signal light to 810nm, and the light intensity to 1W / cm 2 , the pump light wavelength is 532nm, and the light intensity is 10MW / cm 2 . According to the quasi-phase matching condition, the reciprocal lattice vector provided by the periodic structure of the first and fourth parts is used to compensate the wave vector mismatch of the frequency up-conversion, and the length of each cycle is set l 1 =7.45μm; the reciprocal lattice vector provided by the periodic structure in the second part is used to compensate the wavevector mismatch of the polarization coupling of the signal light, and the period length l 2 =9.88μm; the reciprocal lattice vector provided by the periodic structure in the third part is used to compensate the wavevector mismatch of the idler frequency optical polarization coupling, and the period length l 3 =20.48 μm. In order to amplify the signal light energy, set the number of cycles N 1 =1000, the length of the lithium nioba...
Embodiment 2
[0047] Set the wavelength of the signal light to 810nm, and the light intensity to 1W / cm 2 , the pump light wavelength is 532nm, and the light intensity is 10MW / cm 2 . According to the quasi-phase matching condition, the reciprocal lattice vector provided by the periodic structure of the first and fourth parts is used to compensate the wave vector mismatch of the frequency up-conversion, and the period length l is set 1 =7.45μm; the reciprocal lattice vector provided by the periodic structure in the second part is used to compensate the wavevector mismatch of the polarization coupling of the signal light, and the period length l 2 =9.88μm; the reciprocal lattice vector provided by the periodic structure in the third part is used to compensate the wavevector mismatch of the idler frequency optical polarization coupling, and the period length l 3 =20.48 μm. In order to amplify the signal light energy, set the number of cycles N 1 =1000, the length of the lithium niobate opti...
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