Resonant cavity inside-pumped disk laser
A pump laser and resonant cavity technology, applied in the field of optoelectronics, can solve the problems of high cost, increased cost, and complex system of conjugated double paraboloids, and achieve the effects of increasing industrial cost, improving uniformity, and overcoming the reduction of absorption coefficient
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Embodiment 1
[0054] The resonant cavity of the primary laser in Embodiment 1 is a linear cavity, which is the simplest case.
[0055] The gain material 1 of the first-level laser is Nd:YAG, 9 is the pump source of Nd:YAG, 7 is the laser oscillating in the cavity of the first-level laser, the center wavelength is 1064nm, the spherical cavity mirror is 3 pairs of 1064nm high reflection, and the pair of 2um High antireflection. Here, the dichroic mirror is used to prevent the 2um laser generated by the disc 2 from forming parasitic oscillation between the resonant cavities 3-2. Disc 2 is Tm:YAG, cavity mirror 6 is a 2um full reflection mirror, output mirror 5 is a 2um partial reflection mirror, the function of output mirror 5 is to output 2um laser from the system, and 13 is a power meter, which is used to monitor the primary laser cavity The size of the power within.
[0056] In the experiment, we adjusted the angle of the reflector 3 to make the laser 7 resonate between the resonator 2 an...
Embodiment 2
[0058] When the absorption coefficient of the disk 2 in the embodiment 1 is so low that the pump light absorbed by the disk 2 is not enough to generate laser light, the V-type pumping method in the embodiment 2 can simply solve this situation.
[0059] The gain material 1 of the first-level laser is Nd:YAG, 9 is the pump source of Nd:YAG, 7 is the laser oscillating in the cavity of the first-level laser, the center wavelength is 1064nm, the spherical cavity mirror is 3 pairs of 1064nm high reflection, and the pair of 2um High antireflection. The dichroic mirror is used here to prevent the 2um laser generated by the disc 2 from forming parasitic oscillation between the resonant cavities 3-4. Plane mirror 4 is a 1064nm full mirror disc. 2 is Tm: YAG, the cavity mirror 6 is a 2um full reflection mirror, the output mirror 5 is a 2um partial reflection mirror, the function of the output mirror 5 is that the system outputs 2um laser, and 13 is a power meter, which is used to monito...
Embodiment 3
[0063] When the pumping power density of the first-stage laser in embodiment 1 and embodiment 2 is too low, so that the absorption coefficient of the disc 2 is too low to generate laser light, multiple first-stage lasers in embodiment 3 are connected in series The intracavity pumping scheme can solve this situation.
[0064] The gain material 1 of the primary laser is Nd:YAG, 9 is the pump source of Nd:YAG, and 7 is the laser oscillating in the cavity of the primary laser, and the center wavelength is 1064nm. Here we use two primary lasers connected in series as the pump source.
[0065] The spherical cavity mirror has 3 pairs of 1064nm high reflection and 2um high anti-reflection. Here, the dichroic mirror is used to prevent the 2um laser generated by the disc 2 from forming parasitic oscillation between the resonant cavities 3-3. 2 is Tm: YAG, the cavity mirror 6 is a 2um full reflection mirror, the output mirror 5 is a 2um partial reflection mirror, the function of the ou...
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