Resonant cavity interior laser breakdown spectrum detection device
A laser breakdown spectrum and detection device technology, applied in the field of spectrum measurement, to achieve the effect of easy ionization and high breakdown power
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Embodiment 1
[0030] Such as figure 1 Shown is the basic structure diagram of this embodiment.
[0031] Inside the housing 1 is the structure of a Nd:YAG solid-state laser. A laser diode 2-1 is placed on a radiator 2-2 and a thermoelectric cooler (Thermoelectric Cooler, TE) 2-3. The pumping light A- 1 A group of concentrating devices 2-4 focus on the Nd:YAG crystal rod 3-1; the laser diode 2-1 emits laser light of about 810nm, and the Nd:YAG crystal rod 3-1 is near the end face of the laser diode 2-1 Coated with a film with high transparency to 810nm and high reflection to 1064nm, the rear cavity mirror as the output mirror is a concave mirror 3-2 with a radius of curvature of 5cm, and the concave mirror 3-2 is coated with a For a film with a reflectivity of 95% at 1064nm, the output mirror is a partial reflection mirror at this time; the output mirror and the Nd:YAG crystal rod 3-1 form a resonant cavity 3 . Usually the light intensity in the laser resonator is more than 10 times of the ...
Embodiment 2
[0034] Such as image 3 As shown, the difference between this embodiment and embodiment 1 is that the end of the output mirror near the laser diode 2-1 is coated with a film with a reflectivity of 100% to 1064nm, and the output mirror is a total reflection mirror, so compared to embodiment 1 Said intracavity laser has higher power.
Embodiment 3
[0036] The laser light source of this embodiment uses CO with a wavelength of 10.6um 2 pulsed lasers, such as Figure 4 As shown, the resonant cavity 3 is an F-P cavity formed by a first plane mirror 3-3 and a second plane mirror 3-4 opposite on both sides, and the reflectivity of the opposite face of the two plane mirrors to the 10.6um wavelength incident light B-1 is 99.9%. Change the cavity length by adjusting the distance between the two plane mirrors, when the cavity satisfies the resonance condition u N =(c / 2L)*(N+θ / π), where u N is the interval of the longitudinal mode on the frequency coordinate, c is the speed of light, L is the length of the cavity, N is a natural number, θ is the phase change after the light wave is reflected once, the incident light B-1 resonates in the resonant cavity 3, at this time the cavity The standing wave intensity reaches the maximum, and the light intensity of the oscillating light B-3 is at least 10 times the light intensity of the inp...
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