Tunable chrysoberyl laser pumped by Raman yellow light
A technology of chrysoberyl and lasers, which is applied to lasers, laser components, phonon exciters, etc., can solve problems such as severe thermal load of lasers, quantum loss of pump light and output light, and influence on beam quality and output characteristics, etc., to achieve Small quantum loss, low cost, and improved output performance
- Summary
- Abstract
- Description
- Claims
- Application Information
AI Technical Summary
Problems solved by technology
Method used
Image
Examples
Embodiment 1
[0028] Chrysoberyl (Cr 3+ :BeAl 2 o 4 ) crystal is a kind of laser material with excellent performance. In the study of its absorption spectrum, it is found that the three major axis directions of the crystal have large absorption cross sections in the yellow light band, especially in the E / / b axis. In the direction, there is a strong broad absorption peak centered at 590nm. Therefore, whether it is pumped by polarized light or non-polarized light, pumping chrysoberyl crystals with yellow light can achieve sufficient absorption of pump light. Compared with the previous pumping method of the chrysoberyl laser, it is proposed to use Raman yellow light as the pumping source of the tunable chrysoberyl laser, which is not only low in cost, but also can be realized because it can be aligned with the absorption peak of the chrysoberyl crystal High optical efficiency and small quantum deficit between pump light and output light can improve the output performance of chrysoberyl lase...
Embodiment 2
[0036] The laser gain medium in Embodiment 2 of the present invention adopts a self-Raman crystal, so the Raman crystal can be omitted in the device, and the dispersion prism is selected as the tuning element of the chrysoberyl laser at the same time. The specific structural diagram is as follows figure 2 shown.
[0037] 808nm or 880nm laser diode pumping source 1 emits pump light, which is transmitted through the energy transmission fiber 2 and focused by the coupling lens group 3 to pump the laser gain medium 5; the laser gain medium 5 adopts a-cut Nd:YVO 4 Crystal, the crystal size is 3×3×10mm 3 , the doping concentration is selected to be 0.3at.%; both ends of the laser gain medium 5 are polished, coated with 1064nm fundamental frequency light and 1176nm first-order Stokes Raman light anti-reflection coating, wrapped with indium sheet and placed in a heat sink, using cooling The circulating water system controls the working temperature. The resonator mirror 4 is a flat ...
PUM
Login to View More Abstract
Description
Claims
Application Information
Login to View More 

