Solid laser with adjustable laser output state
A solid-state laser and output state technology, applied in the laser field, can solve the problem that the laser cannot be effectively controlled actively, and achieve the effects of increasing pump light, reducing processing costs, and overcoming weak absorption
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Embodiment 1
[0085] In this embodiment, the disk laser is taken as an example for illustration, as figure 2 As shown, the loss modulation module 9 is an acousto-optic modulator, and the acousto-optic modulator is arranged in the 1030nm laser optical path 10 . Both the first gain medium 2 and the second gain medium 6 are Yb:YAG discs with a thickness of 200um, and the first output mirror 3 has a reflectivity of 99% for 1030nm laser, but a low reflectivity for 1048nm laser. The second output mirror 7 has a reflectivity of 99% for 1048nm laser light and a low reflectivity for 1030nm laser light. Both the first reflection mirror 5 and the second reflection mirror 8 are high reflection mirrors.
[0086] In the test, the pumping light emitted by the 940nm pumping light source 1 is incident on the first gain medium 2 after passing through the multi-pass pumping system to generate 1030nm laser and start to oscillate in the first resonant cavity. Then the second gain medium 6 absorbs the high-po...
Embodiment 2
[0090] In this embodiment, the disk laser is taken as an example for illustration, as Figure 6 As shown, the loss modulation module 9 is an acousto-optic modulator, and the acousto-optic modulator is arranged in the 1048nm laser optical path 10 . Both the first gain medium 2 and the second gain medium 6 are Yb:YAG discs with a thickness of 200um, and the first output mirror 3 has a reflectivity of 99% for 1030nm laser, but a low reflectivity for 1048nm laser. The second output mirror 7 has a reflectivity of 99% for 1048nm laser light and a low reflectivity for 1030nm laser light. Both the first reflection mirror 5 and the second reflection mirror 8 are high reflection mirrors.
[0091] In the test, the pumping light emitted by the 940nm pumping light source 1 is incident on the first gain medium 2 after passing through the multi-pass pumping system to generate 1030nm laser and start to oscillate in the first resonant cavity. Then the second gain medium 6 absorbs the high-po...
Embodiment 3
[0095] In this embodiment, a disk laser is taken as an example for illustration, the loss modulation module 9 is an electro-optic modulator, and the electro-optic modulator is arranged in the 1030nm laser optical path 10 . Both the first gain medium 2 and the second gain medium 6 are Yb:YAG discs with a thickness of 200um, and the first output mirror 3 has a reflectivity of 99% for 1030nm laser, but a low reflectivity for 1048nm laser. The second output mirror 7 has a reflectivity of 99% for 1048nm laser light and a low reflectivity for 1030nm laser light. Both the first reflection mirror 5 and the second reflection mirror 8 are high reflection mirrors.
[0096] In the test, the pumping light emitted by the 940nm pumping light source 1 is incident on the first gain medium 2 after passing through the multi-pass pumping system to generate 1030nm laser and start to oscillate in the first resonant cavity. Then the second gain medium 6 absorbs the high-power 1030nm laser in the ca...
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