Abstract

The growth of the Stokes pulse from spontaneous noise during stimulated Raman scattering of picosecond pump pulses in optical fibers, is investigated by using a Langevin-noise term in the coupled nonlinear Schrodinger equations, which include pump depletion, group-velocity mismatch, fiber dispersion, and self- and cross-phase modulation. The model makes use of the actual Raman-gain spectrum of optical fibers. Numerical simulations are used to examine the average behavior of the Stokes pulse, and shot-to-shot fluctuations that are likely to occur in practice. It is shown that the Raman-induced energy transfer is significantly affected by group-velocity dispersion for pump-pulse widths shorter than 5 ps. Examination of the average temporal width shows that the Stokes pulse is initially as wide as the pump pulse, undergoes a gain induced compression and then rebroadens for distances longer than a walk-off length. The effect of varying pump and fiber parameters is to change the minimum value of the Stokes-pulse width, and the distance at which the minimum occurs. The shot-to-shot energy and pulse-width fluctuations initially increase before being reduced at fiber lengths longer than the walk-off length. The primary effect of dispersive and nonlinear effects is to change the distance beyond which fluctuations decrease. >

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