Berlin : Weierstraß-Institut für Angewandte Analysis und Stochastik
Doi
Abstract
Taking up to fourth order dispersion effects into account, we show that
fiber resonators become stable for large intensity regime. The range of pump
intensities leading to modulational instability becomes finite and
controllable. Moreover, by computing analytically the thresholds and
frequencies of these instabilities, we demonstrate the existence of a new
unstable frequency at the primary threshold. This frequency exists for
arbitrary small but nonzero fourth order dispersion coefficient. Numerical
simulations for a low and flattened dispersion photonic crystal fiber
resonator confirm analytical predictions and opens the way to experimental
implementation