Nonlinear optical crystal material, preparation method and application thereof
A technology of nonlinear optics and nonlinear crystals, applied in the field of nonlinear optical materials, can solve the problems of unsatisfactory comprehensive performance, low laser damage threshold, large crystal growth, etc., and achieve excellent infrared nonlinear optical performance and excellent infrared nonlinear Excellent optical properties and crystallinity
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Embodiment 1
[0030] The preparation of embodiment 1 powder crystal sample
[0031] Ga 2 o 3 , boron and selenium according to Ga 2 o 3 :B:Se=1:2:3 molar ratio, mixed with flux, ground evenly, placed in a quartz reaction tube, vacuumed to 10 -2 Pa and use a hydrogen-oxygen flame to melt and seal the quartz reaction tube. Put the quartz reaction tube into a high-temperature furnace, heat it to the solid melting temperature, and keep it for a period of time. Then the temperature is programmatically lowered to 300°C at a speed not exceeding 5°C / hour, then the heating is stopped, cooled naturally to room temperature, washed with distilled water to remove flux, and dried to obtain the nonlinear optical crystal material.
[0032] The sample number, raw material type, flux type and dosage, solid melting temperature and holding time are shown in Table 1.
[0033] Table 1
[0034]
Embodiment 2
[0035] The preparation of embodiment 2 single crystal sample
[0036] Raw material type and proportioning are the same as sample 1 in embodiment 1 # , the raw materials and flux are ground evenly and placed in a quartz reaction tube, vacuumed to 10 -2 Pa and use a hydrogen-oxygen flame to melt and seal the quartz reaction tube. Put the quartz reaction tube into a high-temperature furnace, heat it to 650°C, keep it for 5 hours, then raise the temperature to 950°C and keep it for 24 hours, then cool it down to 300°C at a speed of no more than 5°C / hour, then stop heating and let it cool naturally to room temperature, washed with distilled water to remove flux KI, and dried to obtain a single crystal sample of the nonlinear optical crystal material, which is designated as sample 4 # .
Embodiment 3
[0037] The structural characterization of embodiment 3 sample
[0038] sample 1 # ~4 # The X-ray powder diffraction phase analysis (XRD) was carried out on the MiniFlex II X-ray diffractometer of Rigaku Company, Cu target, Kα radiation source (λ=0.154184nm). The result shows that the sample 1 prepared by embodiment 1 and 2 # ~4 # Both are samples of high purity and high crystallinity, typical representatives such as figure 1 Medium sample 4 # The XRD spectrum. sample 1 # , Sample 2 # , sample 3 # The XRD spectrum result and figure 1 The same, that is, the same diffraction peak position and shape, and the relative peak intensity fluctuates within ±5%. Description Sample 1 # ~4 # have the same crystal structure.
[0039] Sample 4 # The X-ray single crystal diffraction was carried out on a Mercury CCD type single crystal diffractometer, Mo target, Kα radiation source (λ=0.07107nm), test temperature 293K. And through Shelxtl97 for structural analysis. The theoretic...
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