KrF laser-induced photobleaching effects in O2 planar laser-induced fluorescence signals: Experiment and model

Applied Optics

Volumn 36, Issue 12, 1997, Pages 2675-2683

  Nguyen, Quang Viet ^a   Paul, Phillip H ^a  

^a SANDIA NATIONAL LABORATORIES   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0003428351     PISSN: 1559128X     EISSN: 21553165     Source Type: Journal    
DOI: 10.1364/AO.36.002675     Document Type: Article

References (22)

1. 2 (v" = 6 or 7) in an automobile spark-ignition engine using a tunable KrF excimer laser, ” Appl. Opt. 31, 7684-7689 (1992).
2. M. Verslüis, M. Boogarts, R. Klein-Doüwel, B. Thus, W. de Jongh, A. Braam, J. J. ter Meülen, W. L. Meerts, and G. Meijer, “Laser-induced fluorescence imaging in a 100 kW natural gas flame, ” Appl. Phys. B 55, 164-170 (1992).
3. T. M. Qüagliaroli, G. Laüfer, S. D. Hollo, R. H. Krauss, R. B. Whitehurst III, and J. C. McDaniel, “Planar KrF laser-induced OH fluorescence imaging in a supersonic combustion tunnel, ” J. Propul. Power 10, 377-381 (1994).
4. H. Neij and M. Alden, “Application of two-photon laser-induced fluorescence for visualization of water vapor in combustion environments, ” Appl. Opt. 33, 6514-6523 (1994).
5. P. Andresen, A. Bath, W. Groger, H. W. Lülf, G. Meijer, and J. J. ter Meulen, “Laser-induced fluorescence with tunable excimer lasers as a possible method for instantaneous temperatüre field measurements at high pressures: checks with an atmospheric flame, ” Appl. Opt. 27, 365-378 (1988).
6. + (v' = 3) obtained from optical-optical double-resonance linewidth measurements, ” J. Chem. Phys. 95, 7054-7060 (1991).
7. E. W. Rothe, Y.-W. Gü, and G. P. Reck, “Laser induced predissociative fluorescence: Dynamics and polarization and the effect of lower-state rotational energy transfer on quantitative diagnostics, ” Appl. Opt. 35, 934-947 (1996).
8. 2 fluorescence, ” Appl. Opt. 34, 5501-5512 (1995).
9. V. Sick and M. Szabadi, “Einstein coefficients for oxygen B-X transitions used in LIF experiments with tunable KrF excimer lasers, ” J. Quant. Spectrosc. Radiat. Transfer 54, 891-898 (1995).
10. 33Y„~ (v = 0, 2), ” J. Chem. Phys. 98, 5117-5133 (1993).
11. Q. V. Nguyen, R. W. Dibble, C. D. Carter, G. J. Fiechtner, and R. S. Barlow, “Raman-LIF measurements of temperature, major species, OH, and NO in a methane-air Bunsen flame, ” Combus. Flame 105, 499-510 (1996).
12. J. W. Daily, “Use of rate-equations to describe laser excitation in flames, ” Appl. Opt. 16, 2322-2327 (1977).
13. R. P. Lucht, D. M. Sweeney, and N. M. Laurendeau, “Balanced cross-rate model for saturated molecular fluorescence in flames using nanosecond pulse length laser, ” Appl. Opt. 19, 3295-3300 (1980).
14. D. H. Campbell, “Collisional effects on laser-induced fluorescence measurements of hydroxide concentrations in a combustion environment. 1. Effects for v' = 0 excitation, ” Appl. Opt. 23, 689-703 (1984).
15. G. Zizak, F. Cignoli, and S. Benecchi, “A complete treatment of a steady-state four-level model for the interpretation of OH laser-induced fluorescence measurements in atmospheric pressure flames, ” Appl. Phys. B 51, 67-70 (1990).
16. J. M. Seitzman and R. K. Hanson, “Comparison of excitation techniques for quantitative fluorescence imaging of reacting flows, ” AIAA J. 31, 513-519 (1993).
17. M. Legentil, S. Pasquirs, V. Puech, and R. Riva, “Spectroscopic diagnostics of the onset of discharge instabilities in a XeCl phototriggered laser, ” Appl. Phys. B 58, 515-517 (1994).
18. K. P. Huber and G. Herzberg, Molecular Spectra and Molecular Structure IV. Constants of Diatomic Molecules (Van Nostrand Reinhold, New York, 1979), pp. 496-498.
19. 3Y-state, ” Chem. Phys. Lett. 249, 335-340 (1996).
20. 2, ” J. Quant. Spectrosc. Radiat. Transfer 36, 209-232 (1986).
21. 3Y* transitions, ” Can. J. Phys. 44, 2944-2946 (1966).
22. +(v = 0) OH, ” Appl. Opt. 25, 4086-4095 (1986).