A slab-pumped mid-infrared optical parametric oscillator
A parametric oscillator, pump light technology, applied in lasers, laser parts, phonon exciters, etc., can solve the problem of difficulty in obtaining high-power mid-infrared laser output, deterioration of mid-infrared laser beam quality, and limiting laser pump power. and other problems, to achieve the effect of achieving high-power mid-infrared laser output, reducing damage probability, and high pump power
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specific Embodiment approach 1
[0024] The seed laser 1 uses a fiber-coupled 808nm diode laser to end-pump an Nd-doped gain crystal to obtain several watts and a beam quality factor of M in a folded resonator. 2 Fundamental mode 1.064μm output of <1.5. The pulse modulation is realized through the acousto-optic Q switch in the cavity. By adjusting the gain, cavity length, Q switch parameters, etc., the pulse frequency of the seed laser can be adjusted from thousands of hertz to tens of kilohertz, and the pulse width is tens of nanoseconds to hundreds of nanoseconds. Seconds can be designed. Through the selection of the Nd crystal, the control of the polarization device in the resonator, etc., the seed laser can achieve linear polarization output to achieve the phase matching of the subsequent OPO system.
[0025] The slab amplifier system 2 is mainly composed of a beam shaping and transmission system, an isolation system, and a side-pumped Nd slab amplifier module. The beam shaping and transmission system i...
specific Embodiment approach 2
[0032] combine figure 1 and figure 2 Describe this embodiment. The difference between this embodiment and Embodiment 1 is that the seed laser 1 adopts a linear cavity system composed of a rod-shaped side pump module, such as figure 2 hint. In the figure, the pump total reflection mirror 8 is coated with a 1.064 μm total reflection film, and the pump output mirror 12 is coated with a 1.064 μm laser partial reflection film, which constitute the resonant cavity of the seed laser. The acousto-optic Q switch 9 realizes the pulse modulation of the seed laser, and the repetition frequency is adjustable from thousands of hertz to tens of kilohertz. The gain medium of the rod side pumping module 10 is a uniformly doped Nd:YAG rod with a diameter of 2 mm and a length of 106 mm, and an 808 nm diode laser chip is uniformly irradiated on the side of the rod. The polarizer 11 is placed in the resonant cavity to ensure that the seed laser achieves linearly polarized output, thereby achi...
specific Embodiment approach 3
[0033] combine figure 1 This embodiment is described. The difference between this embodiment and Embodiments 1 and 2 is that a 1 mm pulsed fiber laser is used as the seed laser 1 , and parameters such as repetition frequency, pulse width, and beam quality are similar to those in Embodiment 1.
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