Rahman K Arafat, Athmanathan Venkat, Slipchenko Mikhail N, Meyer Terrence R, Roy Sukesh
Appl Opt. 2019 Sep 20;58(27):7458-7465. doi: 10.1364/AO.58.007458.
Broadband femtosecond (fs) two-photon laser-induced fluorescence (TP-LIF) of the BΣ←XΣ, Hopfield-Birge system of carbon monoxide (CO) is believed to have two major advantages compared to narrowband nanosecond excitation. It should (i) minimize the effects of pressure-dependent absorption line broadening and shifting, and (ii) produce pressure-independent TP-LIF signals as the effect of increased quenching due to molecular collisions is offset by the increase in number density. However, there is an observed nonlinear drop in the CO TP-LIF signal with increasing pressure. In this work, we systematically investigate the relative impact of potential deexcitation mechanisms, including collisional quenching, forward lasing, attenuation of the source laser by the test cell windows or by the gas media, and a 2+1 photoionization process. As expected, line broadening and collisional quenching play minor roles in the pressure-scaling behavior, but the CO fs TP-LIF signals deviate from theory primarily because of two major reasons. First, attenuation of the excitation laser at high pressures significantly reduces the laser irradiance available at the probe volume. Second, a 2+1 photoionization process becomes significant as the number density increases with pressure and acts as a major deexcitation pathway. This work summarizes the phenomena and strategies that need to be considered for performing CO fs TP-LIF at high pressures.
与窄带纳秒激发相比,一氧化碳(CO)的BΣ←XΣ霍普菲尔德 - 比尔格体系的宽带飞秒(fs)双光子激光诱导荧光(TP - LIF)被认为有两个主要优点。它应该(i)将压力依赖性吸收线展宽和位移的影响降至最低,并且(ii)由于分子碰撞导致的猝灭增加的影响被数密度的增加所抵消,从而产生与压力无关的TP - LIF信号。然而,观察到CO的TP - LIF信号随压力增加呈非线性下降。在这项工作中,我们系统地研究了潜在去激发机制的相对影响,包括碰撞猝灭、前向激射、测试池窗口或气体介质对源激光的衰减以及2 + 1光电离过程。正如预期的那样,线展宽和碰撞猝灭在压力标度行为中起次要作用,但CO的fs TP - LIF信号偏离理论主要有两个主要原因。首先,高压下激发激光的衰减显著降低了探针体积处可用的激光辐照度。其次,随着数密度随压力增加,2 + 1光电离过程变得显著,并成为主要的去激发途径。这项工作总结了在高压下进行CO的fs TP - LIF需要考虑的现象和策略。