Abstract
Raman fiber lasers (RFLs) are light sources made with long cavities in which a very large number of modes (up to 106) interact through linear (dispersive) and nonlinear effects. They are good candidate to observe turbulent-like behaviors [1,2]. The generation of the multiple cavity modes in RFLs is now commonly described from a complex Ginzburg-Landau equation which has been analyzed from the weak-turbulence theory.
© 2011 Optical Society of America
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