Resonantly enhanced two‐photon photoionization of NO in an atmospheric flame

Molecular multiphoton ionization experiments are reported for the first time in a flame environment. The resonantly enhanced two‐photon photoionization spectrum of NO from 270 to 317 nm in an atmospheric pressure H2/air/N2O flame is essentially identical with respect to both line position and intensity to that which is predicted for the one‐photon absorption to the intermediate A state. A model is developed here which accounts for this result by including rates for collisional repopulation of the laser depleted state. Based on this model, the rotational transfer rate constant for NO is estimated to be ⩾4×109 s−1 in the flame, corresponding to a cross section of ∼70 A2. It is found that the photoionization spectra obtained in this work have far better signal‐to‐noise and resolution than those reported for NO in flames using laser‐induced fluorescence methods and that the estimated detection limit for NO is 1 ppm.

[1]  Lester T. Earls Intensities inΠ2−Σ2Transitions in Diatomic Molecules , 1935 .

[2]  C. Ng,et al.  Photoionization with molecular beams. I. Autoionization structure of nitric oxide near the threshold , 1976 .

[3]  C. F. Curtiss,et al.  Molecular Theory Of Gases And Liquids , 1954 .

[4]  M. Asscher,et al.  Efficient quenching of nitric oxide Rydberg states: A two photon excitation study , 1979 .

[5]  Tucker Carrington,et al.  Rotational, Vibrational, and Electronic Energy Transfer in the Fluorescence of Nitric Oxide , 1963 .

[6]  J. Tatum Interpretation of Intensities in Diatomic Molecular Spectra , 1967 .

[7]  R. J. M. Bennett,et al.  Hönl–London Factors for Doublet Transitions in Diatomic Molecules , 1970 .

[8]  H. Ory,et al.  Franck-Condon Factors for the no Beta and Gamma Band Systems. , 1964 .

[9]  N. Laurendeau,et al.  Two-level model for near saturated fluorescence in diatomic molecules. , 1979, Applied optics.

[10]  V. Vaida,et al.  Effects of nonresonant ionization on multiphoton ionization line shapes , 1981 .

[11]  G. E. Leroi,et al.  Photoionization mass spectrometric study of NO. A closer look at the threshold region , 1973 .

[12]  T. Hollander Photometric measurements on the deviations from the equilibrium state in flames. , 1967 .

[13]  W. Mallard,et al.  Absorption spectra of metal oxides using optogalvanic spectroscopy , 1978 .

[14]  Philip J. M. Johnson,et al.  Rate equation modelling of molecular multiphoton ionization dynamics , 1980 .

[15]  William Klemperer,et al.  Energy transfer in monochromatically excited nitric oxide: A2Σ+ and B2Π , 1973 .

[16]  K. Watanabe,et al.  Absorption coefficient and photoionization yield of NO in the region 580-1350 A. , 1967, Applied optics.

[17]  M. Pryce,et al.  Nonlinear resonant photoionization spectra of molecular iodine , 1977 .

[18]  P. E. Rouse,et al.  The β and γ bands of nitric oxide observed during the flash photolysis of nitrosyl chloride , 1971 .

[19]  R. W. Nicholls,et al.  Absolute oscillator strength measurements of the (υ′ = 0, υ′ = 0–3) bands of the (A2Σ-X2Π) γ-system of nitric oxide , 1972 .

[20]  D. Crosley,et al.  Energy transfer in A 2Σ+ OH. I. Rotational , 1977 .

[21]  Allan C. G. Mitchell,et al.  Resonance radiation and excited atoms , 1934 .

[22]  M. Cottereau,et al.  Study of the collisional lifetime of hydroxyl (2Σ+, ν′ = 0) radicals in flames by time-resolved laser-induced fluorescence , 1981 .

[23]  A. Hayhurst,et al.  Kinetics of collisional ionization of alkali metal atoms and recombination of electrons with alkali metal ions in flames , 1973 .

[24]  P. Fairchild,et al.  Pressure dependence of fluorescence quantum yields and collision-induced rotational relaxation of single rotational , 1981 .

[25]  J. Whitten,et al.  Multiphoton ionization spectroscopy: A theoretical analysis of the NO spectrum , 1978 .

[26]  N. Laurendeau,et al.  Balanced cross-rate model for saturated molecular fluorescence in flames using a nanosecond pulse length laser. , 1980, Applied optics.

[27]  R. Bernstein,et al.  Resonance‐enhanced multiphoton ionization and fragmentation of molecular beams: NO, I2, benzene, and butadiene , 1979 .

[28]  Philip J. M. Johnson Molecular multiphoton ionization spectroscopy. , 1980, Applied optics.

[29]  A. Puretzky,et al.  Selective photoionization of atoms by laser radiation and its applications , 1977 .

[30]  H. Zacharias,et al.  Two-photon excitation of NO(A2Σ+; ν′ = 0,1,2) and radiation lifetime and quenching measurements , 1976 .

[31]  M. J. Pilling,et al.  Fluorescence of nitric oxide. Part 7.—Quenching rates of NO C2Π(v= 0), its rate of radiation to NO A2Σ+, energy transfer efficiencies, and mechanisms of predissociation , 1970 .

[32]  H. Zacharias,et al.  State selective step-wise photoionization of NO with mass spectroscopic ion detection , 1980 .

[33]  J. O. Berg,et al.  Rotational redistribution effect on saturated laser-induced fluorescence. , 1979, Applied optics.

[34]  Ian W. M. Smith,et al.  Fluorescence of nitric oxide. Part 1.—Determination of the mean lifetime of the A2Σ+ state , 1963 .

[35]  F. Gilmore Potential energy curves for N2, NO, O2 and corresponding ions , 1965 .

[36]  R. Barnes,et al.  Nitric oxide measurements in a flame by laser fluorescence. , 1980, Applied optics.

[37]  H. Ory Franck—Condon Factors and Electronic Oscillator Strengths for Nitric Oxide Ultraviolet Band Systems , 1964 .

[38]  W. Mallard,et al.  Mobility measurements of atomic ions in flames using laser-enhanced ionization , 1982 .

[39]  H. O. Kneser,et al.  Relaxation of Nitric Oxide in Mixtures with Argon , 1967 .

[40]  Micha Asscher,et al.  Two-photon excitation of nitric oxide to levels near and above the dissociation limit , 1978 .

[41]  Philip J. M. Johnson,et al.  Two‐ and three‐photon resonances in the four‐photon ionization spectrum of nitric oxide at low temperature , 1978 .

[42]  N. Elander,et al.  Direct Measurements of Lifetimes of Low-lying Excited Electronic States in Nitric Oxide , 1974 .

[43]  D. Crosley Collisional Effects On Laser-Induced Fluorescence Flame Measurements , 1981 .

[44]  A. Pery-Thorne,et al.  Absolute oscillator strength of the (0.0) band of the gamma system of nitric oxide by the hook method , 1970 .

[45]  Y. Ono,et al.  Higher resolution photoionization study of NO near the threshold , 1980 .

[46]  M. Cottereau,et al.  Time resolved study of rotational energy transfer in A 2Σ+(ν′ = 0) state of OH in a flame by laser induced fluorescence , 1981 .

[47]  H. Bauer,et al.  Relaxation of the Vibrational, Electronic, and Rotational Degrees of Freedom of the NO Molecule , 1965 .

[48]  P. Gürtler,et al.  Autoionization structure of nitric oxide (NO) at the first ionization limit , 1978 .

[49]  D. Keefer,et al.  Note of correction: Broadening of NO γ-band lines , 1980 .

[50]  A. Zewail Advances in Laser Chemistry , 1978 .

[51]  O. B. D'azy,et al.  No fluorescence decay from low-lying electronic states excited into single vibronic levels with synchrotron radiation , 1975 .

[52]  L. Dodge,et al.  Errors in reported values for the collisional broadening parameters for nitric oxide γ(0,0) band , 1980 .

[53]  G. Bethke Oscillator Strengths in the Far Ultraviolet. I. Nitric Oxide , 1959 .

[54]  R. W. Nicholls,et al.  Application of dispersion techniques to molecular band intensity measurements. II. Oscillator strength of the (0,0) band of NO-γ (A2 Σ-x2 Π ) system , 1972 .