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In this paper we present procedures for the extraction of laser rate equation parameters.
Based on laser rate equations, we analyzed pulse control of this type of laser.
Traditionally, a separate thermal rate equation, in conjunction with the laser rate equation model is used to describe the thermal behavior [IEEE J. Quant.
The model is based on the self-consistent solution of the Schrödinger and Poisson equations using a one-dimensional scattering rate approach, which includes the laser rate equations.
In [7], the intensity noise in semiconductor lasers has been analyzed using a systematic technique, where the Langevin noise sources have been obtained and the laser rate equations have been derived.
An estimation based on laser rate equations shows that with 960 W pumping power, more than 600 W output power (optical efficiency of 66%) can be extracted from the designed system.
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Lifetimes for each pixel were recorded using time correlated single photon counting (TCSPC) circuitry (SPC-830, Becker & Hickl GmbH), keeping count rates below 1% of the laser repetition rate to prevent pulse pile-up.
Commercially available sources with high repetition rates (>50 KHz) and high enough pulse energy (~4 μJ) to enable laser repetition rate limited FLIM imaging are readily available.
The crack densities increase with laser scan rate.
The laser repetition rate and RMS of the range residuals are given.
Reducing the laser repetition rate distributes the available energy over fewer pulses.
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