Longitudinal mode drift compensation device and method for laser
A technology for drift compensation and lasers, applied to the structure/shape of lasers, laser components, and optical resonators, can solve problems such as high cost, complex structure, and high technical requirements, and achieve low cost, complex structure, and technical difficulty low effect
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Embodiment 1
[0075] Such as image 3 The laser longitudinal mode drift compensation device shown is specifically a device for long-term stability of the longitudinal mode of the uncoated FP laser with closed-loop control Brewster angle incidence. The device includes: etalon FP1-01, the first Cavity mirror 2-01, second cavity mirror 2-02, third cavity mirror 2-03, wavelength meter 4, central control computer 5, electric turntable and driver 6. It can be seen that the resonant cavity in this embodiment is an annular cavity, and the etalon FP1-01 is an uncoated etalon.
[0076] Specifically, the wavelength meter 4 detects the wavelength of the output laser of the resonator, and the central control computer 5 obtains the longitudinal mode drift of the resonator according to the wavelength of the output laser, and generates a feedback signal to the electric turntable and the motor according to the longitudinal mode drift. The driver 6, the electric turntable and the driver 6 adjust the angle o...
Embodiment 2
[0088] Such as Figure 4 The shown laser longitudinal mode drift compensation device is specifically a closed-loop controlled Brewster angle incident uncoated FP laser injection locking device, which includes: etalon FP1-01, first cavity mirror 2 -01, second cavity mirror 2-02, third cavity mirror 2-03, total reflection mirror 3, wavelength meter 4, central control computer 5, electric turntable and driver 6, monolithic non-planar ring cavity laser 7. Among them, the etalon FP1-01 is an uncoated etalon.
[0089] In this embodiment, the total reflection mirror 3 is used to totally reflect the laser output from the resonator to the wavelength meter 4 .
[0090] Wherein, the thickness of the etalon FP1-01 is less than 1 mm, and the material of the etalon FP1 can be quartz, anhydrous quartz, JGS1, etc.; the etalon FP1-01 in this embodiment uses quartz glass with a thickness of 0.7 mm.
[0091] The size of the etalon FP1-01 is Φ25mm×0.7mm.
[0092] In this embodiment, the first ...
Embodiment 3
[0103] Such as Figure 5 The laser longitudinal mode drift compensation device shown is specifically a device for long-term stability of the longitudinal mode of the laser with a closed-loop control of 0-degree incident FP coated with a high-transparency film. The device includes: etalon FP1-02, the first Cavity mirror 2-01, second cavity mirror 2-02, third cavity mirror 2-03, wavelength meter 4, central control computer 5, electric turntable and driver 6. It can be seen that, in this embodiment, the resonant cavity is a ring cavity, and the incident angle of light in the resonant cavity to the etalon FP1-02 is 0 degree.
[0104] Wherein, etalon FP1-02, preferably, etalon FP1-02 thickness is less than 1mm, and described etalon FP1-02 material can be quartz, anhydrous quartz, JGS1 etc.; The etalon FP1-02 in the present embodiment selects 0.7mm thick quartz glass.
[0105] Wherein, the size of the etalon FP1-02 is Φ25mm×0.7mm; as Figure 5 As shown, the incident angle of the ...
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