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As the intensity of the pulse grows, and the phase shift in the auxiliary cavity becomes greater than TT/2, this operation can be accomodated by filtering so that the total change of phase shift across the pulse returned by the auxiliary cavity does not exceed TT. The bias phase has to be just right. This means of course that CCM or APM operation with an auxiliary cavity calls for a feedback arrangement that stabilizes the bias phase against random drifts of the cavity lengths. Such feedback may not be necessary if the interferometeric structure that changes phase modulation into amplitude modulation is part of the main resonator.

A. Haus tive pulse modelocking is achieved when the pulses are far from solitonlike as they pass around the system. They may behave like solitons only on the average^. The new thinking triggered by this approach should be helpful in designing new short-pulse all-fiber lasers. 10 Performance of some APM and KLM systems Rapid progress has been made in recent years in the generation of even shorter pulses using the APM and KLM principles. 2 give some recent advances in the generation of short pulses.

The SAM and SPM coefficients per pass must be evaluated, taking the change of the pulse shape during one transit into account. If the effect of the nonlinearity is small, one may still define the 7 and 8 coefficients as perturbations on the pulse. 27. Location of minimum pulse width in a dispersion compensated ring. minimum pulse width in the loop, because the average pulse profile depends upon it. The pulse polarization rotates across the pulse profile proportionally to the intensity averaged around the loop.

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