Method and device for laser coherence length continuous adjustment
A technology of coherence length and laser, applied in the laser field, can solve the problems of small adjustment range and insufficient stability, and achieve the effect of stable performance and compact structure
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[0043] According to another preferred embodiment of the present invention, the grating is a blazed grating placed in a Littman-Metcalf grazing incidence structure. At this time, the grating can simultaneously obtain large dispersion and low material surface reflectivity, and the grating dispersion item can be simplified for:
[0044] ( ∂ θ G ∂ λ ) G = sin α - sin β λ cos α - - - ( 4 )
[0045] For the above embodiment, by adjusting the rotation and translation device of the grating, it can be ensu...
no. 1 example
[0053] figure 1 It is a structural schematic diagram of the first embodiment of the device for continuously adjusting laser coherence length according to the present invention. Such as figure 1 As shown, the device uses an 808nm semiconductor laser as the laser pumping source 000 of the device in this embodiment.
[0054] The device of this embodiment includes a laser resonant cavity, which contains a prism group composed of sequentially cascaded first optical lens 101, laser gain medium 200, first, second and third right-angle triangular prisms 301, 302, 303 and Blaze grating 400.
[0055] The first optical lens 101 adopts a flat mirror that partially reflects the laser near 1064nm as the output end of the laser.
[0056] Laser gain medium 200 adopts Nd:YVO 4 Crystals used to provide laser gain.
[0057] The first, second, and third rectangular prisms 301, 302, and 303 are placed in an "up-up-down" structure, forming a prism group as a laser beam expander / shrinker device...
no. 2 example
[0064] figure 2 It is a structural schematic diagram of the second embodiment of the device for continuously adjusting laser coherence length according to the present invention. Such as figure 2 As shown, the device also uses an 808nm semiconductor laser as the laser pumping source 000 of the device in the second embodiment.
[0065] The device in this embodiment includes a laser resonant cavity, which contains a third optical lens 103 , a laser gain medium 200 , a frequency doubling crystal 201 and a fourth optical lens 104 cascaded in sequence.
[0066] The third optical lens 103 is used as the incident end of the pumping laser and also as the reflection mirror of the laser resonator, using a flat mirror with high transparency to the laser near 808nm and high reflection to the laser near 1064nm and 532nm.
[0067] Laser gain medium 200 adopts Nd:YVO 4 Crystals used to provide laser gain.
[0068] Frequency doubling crystal 201 adopts KTP crystal, which is used for freq...
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