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Laser-induced incandescence of flame-generated soot on a picosecond time scale

机译:激光诱导的火焰产生的烟尘在皮秒级的白炽度

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This paper presents measurements of time-resolved laser-induced incandescence (LII) from soot recorded on a picosecond time scale. The 532-nm output from a picosecond Nd: YAG laser was used to heat the soot, and a streak camera was used to record the LII signal. The results are compared with data collected on a nanosecond time scale and with a time-dependent model that solves the energy- and mass-balance rate equations. Relative to the laser timing, the picosecond and nanosecond results are very similar. Signals increase during the laser pulse as soot temperatures increase and decrease after the laser pulse. The signal decay rates increase significantly with increasing laser fluence. The LII model gives good agreement with the nanosecond data at fluences ≤ 0.2 J/cm~2 and underpredicts the signal decay rates at higher fluences. The picosecond temporal profiles increase significantly faster and earlier in the laser pulse than predicted by the model. This disagreement between the model and picosecond LII data may be attributable to perturbations to the signal by laser-induced fluorescence from polycyclic aromatic hydrocarbons or other large organic species. The excited state or states responsible for this fluorescence appear to be accessed via a two-photon transition and have an effective lifetime of 55 ps.
机译:本文介绍了以皮秒为单位的烟灰记录的时间分辨激光诱导白炽灯(LII)的测量结果。皮秒Nd:YAG激光器的532 nm输出用于加热烟灰,条纹相机用于记录LII信号。将结果与以纳秒级为单位收集的数据进行比较,并与解决能量和质量平衡速率方程的时间相关模型进行比较。相对于激光定时,皮秒和纳秒的结果非常相似。随着烟尘温度在激光脉冲后升高和降低,信号在激光脉冲期间会增加。信号衰减率随着激光注量的增加而显着增加。在注量≤0.2 J / cm〜2的情况下,LII模型与纳秒数据具有良好的一致性,并且在高注量时低估了信号衰减率。皮秒时间分布图在激光脉冲中的增加明显快于模型预测的速度,并且更早。模型与皮秒LII数据之间的这种差异可能归因于激光诱导的多环芳烃或其他大型有机物种发出的荧光对信号的干扰。引起该荧光的一个或多个激发态似乎是通过两个光子跃迁访问的,有效寿命为55 ps。

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