Method for measuring nonlinear absorption curve of material
A nonlinear absorption and curve technology, used in measurement devices, analytical materials, transmittance measurement, etc., can solve the problems of difficult response of energy meters, limit the measurement range of nonlinear absorption curves, increase the complexity of measurement devices, etc., and achieve high precision. The effect of nonlinear absorption curve measurement, improving the measurement range and improving the measurement accuracy
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Embodiment 1
[0070] The gain medium of the pulse laser is Nd:YLF, and the output fundamental frequency light ω 1 =1053 nm, pulse width τ=50 ps, fundamental frequency spot diameter 0.7cm, horizontal polarization of outgoing laser; crystal frequency doubling system consists of KDP and DKDP crystals, obtained after frequency conversion ω 2 = 263 nm quadruple frequency light; both the dispersion prism and the telephoto lens are ultraviolet high-transmittance components, and the focal length f of the telephoto lens is about 130cm; the material of the beam splitter is fused silica, and the reflectivity is 4%; the sample to be tested is The DKDP crystal with a deuterium content of 66%, the sample thickness h is 0.8 cm, and the sample surface is finely polished; the resolution of the scientific grade CCD camera is 1024 pixels × 1024 pixels, and the size of a single pixel is 13 μm × 13 μm; the attenuation film is Four-fold frequency laser attenuator; the measuring range of the energy meter is...
Embodiment 2
[0084] The implementation of this embodiment is basically the same as that of Embodiment 1, the main difference is that the crystal frequency doubling system is two KDP crystals, which generate ω 2 =351 nm frequency tripled light; the focal length of the telephoto lens is about 140 cm, the distance between the photosensitive surface of the scientific grade CCD camera and the sample to be tested is 104 cm; the attenuation film is a triple frequency laser attenuation film, scientific grade CCD The maximum grayscale of the flare on the camera is 87% of its saturated grayscale. The results show that the transmittance of DKDP crystals decreases nonlinearly with the increase of laser intensity, and compared with the results in Example 1, the nonlinear absorption of DKDP crystals under 351 nm laser irradiation decreases significantly.
Embodiment 3
[0086] The implementation of this embodiment is basically the same as that of Embodiment 1, the main difference is that the gain medium of the pulsed laser is Nd:YAG, and the output fundamental frequency light ω 1 =1064 nm; the crystal frequency doubling system is KDP and DKDP crystals, and the cutting angles of KDP and DKDP crystals are generated for 1064 nm laser ω 2 = 266 nm quadrupled light.
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