KrF laser-induced photobleaching effects in O(2) planar laser-induced fluorescence signals: experiment and model.
暂无分享,去创建一个
[1] R. Barlow,et al. Raman-LIF measurements of temperature, major species, OH, and NO in a methane-air Bunsen flame , 1996 .
[2] Yongwei Gu,et al. Laser-induced predissociative fluorescence: dynamics and polarization and the effect of lower-state rotational energy transfer on quantitative diagnostics. , 1996, Applied optics.
[3] V. Sick,et al. Collisional processes in the O2B3Σu− state , 1996 .
[4] V. Sick,et al. Einstein coefficients for oxygen B-X transitions used in lif experiments with tunable KrF excimer lasers , 1995 .
[5] J C McDaniel,et al. Single-pulse, two-line temperature-measurement technique using KrF laser-induced O(2) fluorescence. , 1995, Applied optics.
[6] M. Aldén,et al. Application of two-photon laser-induced fluorescence for visualization of water vapor in combustion environments. , 1994, Applied optics.
[7] R. Riva,et al. Spectroscopic diagnostics of the onset of discharge instabilities in a XeCl phototriggered laser , 1994 .
[8] T. Slanger,et al. Predissociation linewidths in O2 B 3Σu− (v=0,2) , 1993 .
[9] R. Hanson,et al. Comparison of excitation techniques for quantitative fluorescence imaging of reacting flows , 1993 .
[10] P. Andresen,et al. Identification and imaging of OH (nu'' = O) and O(2) (nu'' = 6 or 7) in an automobile spark-ignition engine using a tunable KrF excimer laser. , 1992, Applied optics.
[11] M. Versluis,et al. Laser-induced fluorescence imaging in a 100 kW natural gas flame , 1992 .
[12] G. Laufer,et al. KrF laser-induced OH fluorescence imaging in a supersonic combustion tunnel , 1992 .
[13] R. Farrow,et al. Predissociation lifetimes of OH A 2Σ+ (V'=3) obtained from optical-optical double-resonance linewidth measurements , 1991 .
[14] F. Cignoli,et al. A complete treatment of a steady-state four-level model for the interpretation of OH laser-induced fluorescence measurements in atmospheric pressure flames , 1990 .
[15] P. Andresen,et al. Laser-induced fluorescence with tunable excimer lasers as a possible method for instantaneous temperature field measurements at high pressures: checks with an atmospheric flame. , 1988, Applied optics.
[16] B. Lewis,et al. Oscillator strengths for the Schumann-Runge bands of 16O18O , 1987 .
[17] N. Laurendeau,et al. Time-resolved fluorescence investigation of rotational transfer in A 2 ∑ + (v = 0) OH , 1986 .
[18] D. H. Campbell. Collisional effects on laser-induced fluorescence measurements of hydroxide concentrations in a combustion environment. 1: Effects for v\prime = 0 excitation. , 1984, Applied optics.
[19] N. Laurendeau,et al. Balanced cross-rate model for saturated molecular fluorescence in flames using a nanosecond pulse length laser. , 1980, Applied optics.
[20] J. Daily,et al. Use of rate equations to describe laser excitation in flames. , 1977, Applied optics.
[21] J. Tatum. HÖNL–LONDON FACTORS FOR 3Σ±−3Σ± TRANSITIONS , 1966 .
[22] Brenton Lewis,et al. Oscillator strengths for the Schumam-Runge bands of 16O2 , 1986 .