Requirements for Tunable Mode and Line Selection by Injection in a TEA-CO2 Laser

R. Menzies, P. Flamant, M. Kavaya
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Abstract

Mode selection in a TEA-CO2 laser cavity through the use of injection techniques provides high peak power single-longitudinal-mode (SLM) pulses with relatively low intensities of injected radiation. Provided the selected mode is near the center of the pressure-broadened TEA-CO2 gain transition, and the frequency proximity requirements are met, as little as 10 μW of injected power is sufficient to effectively produce a single-frequency pulse with peak power of several MW [1]. However, if tunable pulses are desired, the requirements for mode selection as the frequency of the injected radiation is tuned away from the CO2 transition center frequency become more demanding. An analytical treatment of the coupled rate equation for the molecular population densities and for the photon densities yields an expression for the "mode selection time", or the time during which the photon flux in the favored mode is a large fraction (e.g., >90%) of the total photon flux [2]. This expression is valid for values of molecular resonance detuning smaller than the pressure-broadened halfwidth (ΔνL) of the transition.
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TEA-CO2激光器注射可调模式和线路选择的要求
通过使用注入技术在TEA-CO2激光腔中进行模式选择,可以提供具有相对低注入辐射强度的高峰值功率单纵向模式(SLM)脉冲。如果选择的模式靠近压力加宽的TEA-CO2增益过渡的中心,并且满足频率接近要求,则只需10 μW的注入功率就足以有效地产生峰值功率为几MW的单频脉冲[1]。然而,如果需要可调谐脉冲,则随着注入辐射的频率被调谐远离CO2过渡中心频率,对模式选择的要求就变得更加苛刻。对分子密度和光子密度的耦合速率方程进行解析处理,可以得到“模式选择时间”的表达式,即在有利模式下的光子通量占总光子通量的很大一部分(例如>90%)的时间[2]。该表达式适用于分子共振失谐值小于跃迁的压力加宽半宽(ΔνL)。
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