All-solid-state Raman frequency multiplication dark red laser and laser generation method
A deep red, all-solid-state technology, applied in the direction of lasers, laser components, phonon exciters, etc., can solve the problems of high cost, bulky, lack of high performance, etc., achieve high average power and high peak power, and reduce volume and cost, the effect of beam quality purification
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Embodiment 1
[0027] figure 1 It is a schematic diagram of an optical path of an all-solid-state Q-switched Raman frequency-multiplied deep red laser of the present invention. The pump source 1 is a fiber-coupled 880nm semiconductor laser (the fiber diameter is 200 microns, and the numerical aperture is 0.22); the pump light passes through the collimating lens 2 with a focal length of 50 mm and the focusing lens 3 with a focal length of 250 mm in sequence, and then injects into the laser crystal 5 , with a focal spot diameter of 1 mm. Laser crystal 5 chooses 4×4×40mm 3 , 1at.% doped Nd:YLF crystal, coated with 880nm, 1047-1053nm and 1314-1321nm anti-reflection coatings on both ends. The Q-switching device 6 is an acousto-optic Q switch, the ultrasonic frequency is 27.12MHz, the radio-frequency power is 100W, and the two ends are coated with 1314-1321nm anti-reflection film; the acousto-optic Q-switching is used to generate nanosecond pulse laser with high peak power to improve Raman and ...
Embodiment 2
[0030] figure 2 It is a schematic diagram of the optical path of a high-power side-pumped all-solid-state Q-switched Raman frequency-multiplied deep red laser of the present invention. This embodiment is further improved on the basis of Embodiment 1. The difference between it and Embodiment 1 is : The pump source 1 pumps the laser crystal 5 from the side, without the collimator lens 2 and the focusing lens 3; the side pump structure can effectively increase the pump power applied to the laser crystal 5, thereby increasing the output power of the deep red laser.
Embodiment 3
[0032] image 3It is a schematic diagram of the optical path of an all-solid-state continuous Raman frequency-doubling deep red laser of the present invention. This embodiment is further improved on the basis of Embodiment 1. The difference between it and Embodiment 1 is that there is no modulation in the resonant cavity. Q device 6 to achieve continuous deep red laser output.
[0033] In summary, the deep red laser disclosed in the present invention has many advantages such as high output power, good beam quality, simple structure, stable performance, and low cost, and has important applications in the fields of laser display, biophotonics, fluorescence imaging, photodynamic therapy, etc. .
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