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Cr:ZnSe laser (positive GDD)

For modelling, we have chosen the experiment described in Ref. [26] with the following simulation parameters: $ P = (corresponds to 1.5 W absorbed pump power at 1.61 $ \mu$m), output coupling $ \rho=0.01$, and GDD = 3500 fs$ ^2$ (material dispersion of the Cr:ZnSe crystal and acousto-optic modulator). As Kerr-lens mode locking mechanism was of the "soft-aperture" type, the exact value of the $ \sigma $ parameter is unknown. The level of saturable losses $ \gamma$ was estimated from the output power level to be up to two times higher than the losses due to the output coupler. In the simulation, the ranges of $ \gamma$ and $ \sigma $ are 0.01$ \div$0.02 and 5$ \div$10, respectively. Within these ranges, the modelling predicts the stable multipulsing with 2 to 28 pulses simultaneously present in the cavity. The typical pulse duration was 0.3-5 ps, distance between pulses 1 - 15 ps. Figure [*] compares the simulated autocorrelation trace (pulse duration 4.4 ps, pulse distance 11.3 ps) with the experimental autocorrelation signal [26] (pulse duration 4.5 ps, distance 13.5 ps). The result was obtained using $ \gamma = 0.02$ and $ \sigma = 10$ parameters, both within the expected range of parameters and demonstrates validity of the model in the positive GDD regime.

Figure: Simulated and experimental autocorrelations of the multiple pulse Kerr-lens mode-locked Cr:ZnSe laser
\resizebox{0.4\textwidth}{!}{%%.


next up previous
Next: Ti:sapphire laser (negative GDD) Up: Multiple pulse operation Previous: Bounded multiple pulses
V.L. Kalashnikov 2002-12-28
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