Richardson Daniel R, Stauffer Hans U, Roy Sukesh, Gord James R
Appl Opt. 2017 Apr 10;56(11):E37-E49. doi: 10.1364/AO.56.000E37.
A comparison is made between two ultrashort-pulse coherent anti-Stokes Raman scattering (CARS) thermometry techniques-hybrid femtosecond/picosecond (fs/ps) CARS and chirped-probe-pulse (CPP) fs-CARS-that have become standards for high-repetition-rate thermometry in the combustion diagnostics community. These two variants of fs-CARS differ only in the characteristics of the ps-duration probe pulse; in hybrid fs/ps CARS a spectrally narrow, time-asymmetric probe pulse is used, whereas a highly chirped, spectrally broad probe pulse is used in CPP fs-CARS. Temperature measurements were performed using both techniques in near-adiabatic flames in the temperature range 1600-2400 K and for probe time delays of 0-30 ps. Under these conditions, both techniques are shown to exhibit similar temperature measurement accuracies and precisions to previously reported values and to each other. However, it is observed that initial calibration fits to the spectrally broad CPP results require more fitting parameters and a more robust optimization algorithm and therefore significantly increased computational cost and complexity compared to the fitting of hybrid fs/ps CARS data. The optimized model parameters varied more for the CPP measurements than for the hybrid fs/ps measurements for different experimental conditions.
对两种超短脉冲相干反斯托克斯拉曼散射(CARS)测温技术进行了比较,即飞秒/皮秒混合(fs/ps)CARS和啁啾探测脉冲(CPP)飞秒CARS,这两种技术已成为燃烧诊断领域高重复率测温的标准方法。这两种飞秒CARS变体仅在皮秒持续时间探测脉冲的特性上有所不同;在混合飞秒/皮秒CARS中,使用的是光谱窄、时间不对称的探测脉冲,而在CPP飞秒CARS中使用的是高度啁啾、光谱宽的探测脉冲。在温度范围为1600 - 2400 K的近绝热火焰中,使用这两种技术进行了温度测量,探测时间延迟为0 - 30皮秒。在这些条件下,两种技术都显示出与先前报道的值以及彼此相似的温度测量精度和精密度。然而,可以观察到,与混合飞秒/皮秒CARS数据的拟合相比,对光谱宽的CPP结果进行初始校准拟合需要更多的拟合参数和更强大的优化算法,因此计算成本和复杂性显著增加。在不同的实验条件下,CPP测量的优化模型参数变化比混合飞秒/皮秒测量的更大。