A solid-state blue laser
A technology of solid-state lasers and lasers, applied in the field of blue-ray lasers, can solve problems such as limited amplification, difficulty in obtaining high-power laser output, and difficult realization of laser dual oscillation, and achieve high gain and good amplification
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Embodiment 1
[0053] figure 1 Shown: a high-efficiency, amplified solid-state blue laser, including: a base frequency module 1, a frequency doubling crystal 2, a Raman medium 3, a sum frequency crystal 4, and a beam splitter 5. The base frequency module is a solid-state laser with a wavelength of 1 micron, and the laser generated by it is a linearly polarized pulse laser; the frequency doubling module includes at least a frequency doubling crystal, the frequency doubling crystal is coaxial with the base frequency laser, and the base frequency laser generates frequency doubling laser through the frequency doubling crystal. The two ends of the frequency doubling crystal are coated with a film system with high transmittance to the 1 micron band laser and the frequency doubling laser; the stimulated Raman module includes at least the Raman medium, and the laser enters the Raman medium after frequency doubling, because the Raman conversion gain coefficient is related to the incident The square o...
Embodiment 2
[0060] figure 2 Shown: a high-efficiency, amplified solid-state blue laser, including: a fundamental frequency module 1, a frequency doubling crystal 2, a Raman medium 3, a sum frequency crystal 4, a beam splitter 5, and a frequency doubling beam shaping system 7.
[0061] It can be seen from the figure that the difference between this embodiment and Embodiment 1 is that the fundamental frequency laser enters the frequency doubling crystal after being shaped by the frequency doubling beam shaping system. The lens or lens group is used to shape the fundamental frequency laser, so that the fundamental frequency laser entering the frequency doubling crystal has high power density.
Embodiment 3
[0063] image 3 Shown: a high-efficiency, amplified solid-state blue laser, including: a fundamental frequency module 1, a frequency doubling crystal 2, a Raman medium 3, a sum frequency crystal 4, a beam splitter 5, and a Raman beam shaping system 8.
[0064] It can be seen from the figure that the difference between this embodiment and Embodiment 1 is that the fundamental-frequency laser and the frequency-doubled laser enter the Raman medium after being shaped by the Raman beam shaping system. The lens or lens group of the high-transmission film system of the frequency-doubled laser is used to shape the pump laser, so that the pump laser entering the Raman gain cell has a high power density.
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