A large-diameter laser amplifier based on multi-dimensional laser diode stack side pumping
A technology of laser diodes and laser amplifiers, which is applied to lasers, laser components, semiconductor lasers, etc., can solve problems such as the decrease in the gain of the amplified laser, the impact on the quality of the amplified laser beam, and the uneven gain of the pumping region, so as to facilitate troubleshooting problems, improved coupling efficiency, and better beam quality
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Embodiment 1
[0057] Such as figure 2 , image 3 As shown, the large-aperture laser amplifier based on the multi-dimensional laser diode stack side pumping provided by Embodiment 1 of the present invention includes a plurality of pump light source combinations 10 , a working substance 20 and a cooling device 30 . Wherein, each pump light source combination 10 includes a semiconductor laser diode stack 11, a beam shaping unit 13 (11 and 13 are set as one in the figure, of course, 11 and 13 can also be set separately) and a coupling light pipe 12, close to The light outlet of the semiconductor laser diode stack 11 is provided with a beam shaping unit 13 and a coupling light pipe 12 in sequence, wherein the semiconductor laser diode stack 11 is a large-area semiconductor laser diode stack. The shape of the working substance 20 is a regular prism, the upper and lower bases of the regular prism are regular polygons, the upper and lower bases are parallel, and the side length of the regular pol...
example
[0087] l 1 =30mm, the refractive index of air n 1 =1, the working substance is neodymium glass, its refractive index n 2 = 1.53, m = 10 mm.
[0088] The pump light must be totally reflected in the working substance 20, and must satisfy Then there is θ c =40.81°.
[0089] when θ 3 Total reflection will occur at >40.81°.
[0090] The light incident from the left side of the normal, the incident light can be totally reflected, there must be θ 5 ≤40.81°.
[0091] If θ 5 = 30°, θ 2 >10.81°, then θ 1 >16.68°, that is, light with an incident angle greater than 16.68° is totally reflected, and 73.32° of light can be totally reflected.
[0092] If θ 5 =40.81°, θ 2 >0°, then θ 1 >0°, that is, the light with an incident angle greater than 0° will be totally reflected, and the light within 90° will be totally reflected. Since there are two boundary conditions: incident from the left side of the normal, and one side (AB) of the working substance 20, the incident angle of th...
Embodiment 2
[0097] Such as Figure 9 As shown, the difference between embodiment 2 and embodiment 1 is: in embodiment 2, the lower bottom surface of the prism of the working substance 20 is at the upper end, and the upper bottom of the prism is at the lower end, and the laser that needs to be energy amplified passes through the lower end of the prism. The incidence from the bottom surface is opposite to that of the working substance 20 in Embodiment 1. Wherein, the diameter of the working substance 20 is relatively large, and the side length L of the regular polygon under the bottom surface of the regular prism is greater than or equal to 10 mm. The lower bottom surface of the positive prism of the working substance 20 is coated with a high-transmittance film consistent with the wavelength of the laser that needs to be amplified in energy, and is used to transmit the laser that needs to be amplified in energy; The reflective film with the same wavelength of the amplified laser is used to...
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