Full-solid-state single longitudinal mode yellow light laser
A single longitudinal mode and laser technology, which is applied in lasers, laser components, phonon exciters, etc., can solve the problem of sensitivity to changes in pump power or cavity length, single longitudinal mode operation mechanism is easily damaged, and frequency-selective components The production requirements are harsh and other issues, to achieve the effect of eliminating multi-longitudinal mode competition, improving stability and spectral line purity, and small size
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Embodiment 1
[0038] Such as figure 1As shown, in the all-solid-state single longitudinal mode yellow laser of this embodiment, two λ / 4 wave plates are arranged in parallel on both sides of the laser crystal 35, and the Brewster window 343 is arranged between the second λ / 4 wave plate 342 and the splitter. Between the beam mirrors 36, the Brewster window ensures that the P-polarized 1064nm fundamental frequency light has zero reflection loss and prevents the S-polarized light from passing through; in addition, the specific selection of each optical element of the all-solid-state single longitudinal mode yellow laser in this embodiment The type parameters are: LD end pump source 1, laser diode LD provides 808nm pump light, the maximum output power is 20W, and comes with a cooling device; the core diameter of the coupling fiber is Φ200um, the numerical aperture is 0.22, and the collimating and focusing lenses are coated with 808nm Transparent film; a Raman composite resonator composed of the ...
Embodiment 2
[0041] Such as figure 2 As shown, this embodiment is basically the same as Embodiment 1, except that the two λ / 4 wave plates of the all-solid-state single longitudinal mode yellow laser of this embodiment are arranged in parallel on both sides of the Raman crystal 37, Brewster The window 343 is arranged between the second λ / 4 wave plate 342 and the beam splitter 36, wherein the Brewster window 343 window ensures that the P-polarized Stokes light has zero reflection loss and prevents the S-polarized Stokes light from passing through, and the two λ / 4 waves The center wavelength of the slice corresponds to the Stokes light wavelength, and the other optical path propagation processes are exactly the same as those in Embodiment 1, and will not be repeated here.
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