Non-moving type adjustable focal length lens and light beam scanning structure
A beam scanning, mobile technology, applied in the field of laser and optics, can solve the problems of small change, high voltage required, slow speed, etc.
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Embodiment 1
[0023] As shown in Figure 1, 101 is the absorber of specific optical wavelength optical material, 103 wavelength is λ pump light, 104 wavelength is the light to be adjusted by λ1, wherein the optical absorber (101) absorption wavelength is λ pump light (103 ), to λ1 light (104) transmission, 102 is the optical substrate coated with the λ reflective pair 104λ transmissive film. It is known from the laser principle that when the optical element absorbs the pump light, a thermal lens will be formed due to the temperature gradient. For example, when a semiconductor laser pumps a solid laser gain material, a thermal lens is usually formed by the following formula (P409: "Solid Laser Engineering") [US] W. Kirchner, Science Press, 2002)
[0024] f = πkcWp 2 P H ( dn dt ...
Embodiment 2
[0028] Such as Figure 5 As shown, 101 is an optical absorber, 103 is a pump light with a wavelength of λ, and 104 is a light beam to be adjusted. The difference from Embodiment 1 is that the pump light is pumped from the side, and 204 is a converging lens. The optical absorber (101 ) will form a wedge-shaped refractive index change distribution, which can be equivalent to an optical wedge. When the pump power changes, the refractive index changes, so that the beam direction is polarized.
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