Optical parametric oscillator with reflectivity-variable internal cavity
A technology of optical parametric oscillator and reflectivity, which is applied in the laser field, can solve the problems of large beam divergence angle, poor beam quality, and limit the practical application of optical parametric oscillator, and achieve the effect of improving beam quality and reducing beam divergence angle
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Embodiment 1
[0017] As shown in Figure 3(a), the geometric configuration of the intracavity optical parametric oscillator adopts an unstable cavity structure, and the nonlinear crystal 2 is KTP (KTiOPO 4 ), working in a non-critical phase matching mode; the laser crystal 5 uses Nd:YAG, and is excited by a xenon lamp 12 to generate a laser with a wavelength of 1.064 μm; 10 is a passive Q-switched crystal, and 11 is a polarizer. The left side of the output mirror 3 is coated with a 1.57 μm variable reflectance film system, and the right side is coated with a double-layer film with high transmittance for light with a wavelength of 1.57 μm. The variable reflectivity curve of the output mirror 3 adopts figure 2 The 2nd order Gaussian linetype in 6. The output wavelength of Example 1 is around 1.57 μm.
[0018] The structure of the variable reflectivity film system inside the output mirror 3 is shown in Figure 3(b), wherein 15 is a substrate made of K9 glass; 16 is a 1 / 4 wavelength film of zir...
Embodiment 2
[0024] Embodiment 2 The geometric configuration adopts a flat-flat cavity, as shown in Figure 4, the nonlinear crystal 2 is periodically poled lithium niobate; 11 is a polarizer, and the laser crystal 5 is Nd:YAG, and the excitation is provided by a diode laser array 22 , producing a 1.064μm continuous laser. The right side of the middle mirror 1 is coated with a 1.57 μm variable reflectance film system, and the double-layer film on the left side has a high transmittance for light with a wavelength of 1.064 μm. The variable reflectivity curve uses figure 2 The 6th order Gaussian curve in 8. The output wavelength of Example 2 is around 1.57 μm.
[0025] The structure of the variable reflectivity film system on the right side of the intermediate mirror 1 is shown in Figure 4(b), where 15 is a substrate made of K9 glass; 16 is a 1 / 4 wavelength film of zirconium dioxide with a thickness of about 0.20 μm; 17 It is a silicon dioxide 1 / 4 wavelength film with a thickness of about 0...
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