Abstract
A simple analytical model is presented to describe the delay τ <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">c</inf> between flashlamp initiation and laser-pulse onset in the flash-photolysis HF chemical laser. The predictions of the model agree well with experiments concerning the functional dependence of τ <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">c</inf> on pressure, flashlamp intensity, optical cavity loss, and the absolute magnitude of τ <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">c</inf> . This detailed agreement between theory and laser performance has not been achieved in previous chemical laser work. The pulse-delay measurements demonstrate the presence of complete vibrational inversion at the time of laser-pulse initiation. In the Appendixes, the fractional photodissociation of MoF <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">6</inf> is calculated for the experimental geometry used, the effects of flashlamp heating are considered, and a general expression for the temperature dependence of HF laser gain is derived and plotted. A complete bibliography of laser transitions in HF and DF is included.
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