Abstract
Intracavity Raman lasers provide a practical way to access hard to reach wavelengths by transforming the fundamental wavelengths into longer ones through stimulated Raman scattering (SRS) and, using nonlinear conversion processes, up-converting them into the visible, ranging from blue to red [1,2]. In a self-Raman laser, the fundamental and the Raman laser oscillation are both generated in the same crystal, enabling a compact laser cavity with less optical interfaces and subsequent lower losses.
© 2015 IEEE
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