Abstract
Performance data for a continuous-wave hydrogen fluoride (cw HF) chemical laser master oscillator/power amplifier showed that, regardless of the oscillator or resonator used to generate the input beam, the amplification ratio is an inverse function of the input power (intensity) and, for maximum amplification, the peak of the input intensity distribution must be matched to the peak of the zero power gain distribution in the amplifier. The matc/mismatch of the oscillator/amplifier flowfields has a second-order effect on amplifier performance
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