Abstract
For the generation of coherent radiation at short wavelengths, the non-parametric anti-Stokes Raman laser (ASRL-) process represents an interesting alternative to primary laser techniques or conventional nonlinear methods. The process requires a λ-type three level scheme (Fig. 1) and allows frequency up-shifting of pump radiation vp into anti-Stokes radiation vAS.
© 1988 Optical Society of America
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