A Gas Raman Laser Based on Ring Unstable Cavity
A technology of Raman laser and unstable cavity, which is applied in the field of laser, can solve the problems affecting the optical efficiency of the fundamental frequency, and achieve the effects of non-overlapping laser in the cavity, good beam quality, and improved spectral conversion efficiency
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Embodiment 1
[0035] like figure 1 As shown, a gas Raman laser based on an annular unstable cavity includes a fundamental-frequency laser plane reflector 1, a laser gain medium 2, a fundamental-frequency laser plane reflector 3, and a convex lens 4 coated with a fundamental-frequency optical anti-reflection film, Fundamental frequency laser reflecting Raman light anti-reflection plane mirror 5, Raman cell 6, fundamental frequency laser reflecting Raman light anti-reflection plane mirror 7, convex lens 8 coated with fundamental frequency light anti-reflection film, coated with fundamental frequency light anti-reflection film The Brewster angle window 9 of the film; the intracavity laser passes through the fundamental-frequency laser plane reflector 1, the laser gain medium 2, the fundamental-frequency laser plane reflector 3, and the convex lens coated with the fundamental-frequency anti-reflection film in the clockwise direction 4. A plane mirror 5 for fundamental frequency laser reflection...
Embodiment 2
[0045] like figure 2 As shown, on the basis of Embodiment 1, the gas Raman laser of the annular unstable cavity is inserted outside the cavity along the coaxial Raman optical high reflection mirror 10 of the optical axis on the Raman light transmission path, and the Raman laser The Raman light output coupling mirror 11, the reflection surfaces of the Raman light high reflection mirror 10 and the Raman light output coupling mirror 11 have curvature, and share a center of curvature, and the center of curvature coincides with the focal point in the cavity. The Raman light high reflection mirror 10 and the Raman light output coupling mirror 11 constitute a Raman optical resonant cavity, and the length of the resonant cavity is between the curvature radius of the Raman light high reflection mirror 10 and the Raman light output coupling mirror 11. and. Specifically, when the laser is working, the power density of the fundamental frequency light near the focal point and focal depth...
Embodiment 3
[0047] In Embodiment 1 and Embodiment 2, the laser will propagate clockwise and counterclockwise in the form of traveling waves in the resonator, in which the size of the beam is continuously enlarged as a forward wave, and the other is continuously reduced as a backward wave , the existence of the backward wave will lead to the possible existence of standing waves in the cavity, and the most important thing is that it will generate Raman light, but this part of Raman light cannot be used, which will reduce the Raman conversion efficiency. So, if image 3 As shown, on the basis of Example 2, the Brewster corner window 9 coated with the anti-reflection film of the fundamental frequency light is removed, and the gas Raman laser of the annular unstable cavity has a non-Raman light in the cavity The polarizer 12 coated with the anti-reflection film of the fundamental frequency light, the Faraday rotator 13, the polarizer 14, and the optical rotator 15 are sequentially inserted in ...
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