State‐to‐state excitation of NO(A 2Σ+, v′=0,1,2) by N2(A 3Σ+u, v′=0,1,2)

We have determined that the rate coefficient for quenching N2(A 3Σ+u, v′=0) by NO is (6.6±1.0)×10−11 cm3 molecule−1 s−1. Higher levels of N2(A) appear to be quenched with a similar rate coefficient. Separate studies show that the rate coefficient for the excitation of NO(A 2Σ+, v′=0−2) by N2(A 3Σ+u, v′=0) is (10±3)×10−11 cm3 molecule−1 s−1. The apparent discrepancy between the quenching and excitation rate coefficient measurements most likely results from an error in the accepted value of the lifetime N2(A). Our studies indicate that this lifetime is probably about 30% longer than currently believed. We also report rate coefficients for excitation of each of the vibrational levels 0–2 of NO(A) by each of the vibrational levels 0–2 of N2(A) relative to the rate coefficient for excitation of NO(A, v′=0) by N2(A, v′=0).

[1]  P. M. Wood,et al.  Rates of energy transfer from N2A3Σ+u to various molecules. Initial and final quantum states in the transfer to NOX2Π and Hg(61S0), and vibrational relaxation of N2A3Σ+u(v= 1) in helium , 1971 .

[2]  J. A. Beswick,et al.  A distorted wave calculation for electronic energy transfer in molecular collisions. Application to the N2(A 3Σu+)+CO(X 1Σ+) →N2(X 1Σg+) +CO(a 3Π) system , 1979 .

[3]  M. Shaw,et al.  Measurements of thermal-energy ion-neutral reaction rate coefficients for rare-gas ions , 1970 .

[4]  J. Jeffries,et al.  Vibrational relaxation of N2(A3Σu+,υ = 1, 2,3) by CH4 and CF4 , 1983 .

[5]  A. Farragher Ion-molecule reaction rate studies in a flowing afterglow system , 1970 .

[6]  M. Jeunehomme Transition Moment of the First Positive Band System of Nitrogen , 1966 .

[7]  R. W. Carr,et al.  Use of tubular flow reactors for kinetic studies over extended pressure ranges , 1971 .

[8]  D. Shemansky N2 Vegard–Kaplan System in Absorption , 1969 .

[9]  V. McKoy,et al.  Transition moments between excited electronic states of N2 , 1977 .

[10]  M. Cher,et al.  Chemiluminescent Reactions of Excited Helium with Nitrogen and Oxygen , 1969 .

[11]  R. E. Walker Chemical Reaction and Diffusion in a Catalytic Tubular Reactor , 1961 .

[12]  L. G. Piper,et al.  Rate constants for deactivation of N2(A) v′=0,1 by O2 , 1981 .

[13]  N. Carleton,et al.  Lifetime of the Lowest Excited Level of N2 , 1962 .

[14]  D. Stedman,et al.  Chemical applications of metastable argon atoms II. A clean system for the formation of N2(A3σ+u) , 1968 .

[15]  H. Werner,et al.  Accurate ab initio calculations of radiative transition probabilities between the A 3Σ+u, B 3Πg, W 3Δu, B′ 3Σ−u, and C 3Πu states of N2 , 1984 .

[16]  M. Larsson,et al.  Collisional Transfer to the B State in N2 , 1979 .

[17]  L. G. Piper,et al.  Rate constants for deactivation of N2(A 3Σ+u, v′ = 0,1) by O , 1981 .

[18]  A. Mandl,et al.  Quenching of N2(A 3Σ+u) by I2 , 1977 .

[19]  D. Perner,et al.  Rate constants for the quenching of N2 (A 3Σu+, vA = 0 – 8) by CO, CO2, NH3, NO, and O2 , 1974 .

[20]  Y. Öhrn,et al.  A note on the radiative lifetimes of the B 3Πg state of N2 , 1984 .

[21]  R. Heidner,et al.  Kinetic study of N2(B3Πg, υ) quenching by laser-induced fluorescence☆ , 1976 .

[22]  H. Berg,et al.  Storage Technique for Atomic Hydrogen , 1962 .

[23]  A. Broadfoot,et al.  Excitation of N2 and N+2 systems by electrons—I . Absolute transition probabilities , 1971 .

[24]  R. Young,et al.  Experiments on N2(A3Σu+). II. Excitation of NO , 1968 .

[25]  D. Setser,et al.  Energy transfer reactions of N2(A3.SIGMA.u+). 5. Quenching by hydrogen halides, methyl halides, and other molecules , 1980 .

[26]  L. G. Piper,et al.  Einstein coefficients and transition moment variation for the NO(A 2Σ+–X 2Π) transition , 1986 .

[27]  D. Setser,et al.  Decay rates of Ar(4s,3P2), Ar(4s′,3P0), Kr(5s,3P2), and Xe(6s,3P2) atoms in argon , 1978 .

[28]  A. Broadfoot,et al.  Electronic Transition Moment for the N2 Vegard–Kaplan Bands , 1969 .

[29]  D. Stedman,et al.  Chemical Applications of Metastable Argon Atoms. IV. Excitation and Relaxation of Triplet States of N2 , 1970 .

[30]  D. Shemansky,et al.  Lifetime of the N2 Vegard–Kaplan System , 1969 .

[31]  M. Golde Vacuum UV emission by electronically excited N2: The collision-induced N2(a 1Πg′ υ = 0) ↔ N2(a′1Σu−, υ = 0) transition , 1975 .

[32]  G. Diebold,et al.  KINETICS OF THE ATOMIC OXYGEN + MOLECULAR FLUORINE REACTION. A CASE OF LOW REACTIVITY OF ELEMENTAL FLUORINE , 1977 .

[33]  M. Fujii,et al.  Rotational energy transfer in NO (A2Σ+, v = 0 and 1) studied by two-color double-resonance spectroscopy , 1984 .

[34]  J. Cahn,et al.  Metastable measurements in flowing helium afterglow. , 1967 .

[35]  F. Pipkin,et al.  Lifetime measurements of the B 3Πg state of N2 using laser excitation , 1983 .

[36]  M. Golde,et al.  Study of the products of the reactions of N2(A3Σu+): The effect of vibrational energy in N2(A) , 1985 .

[37]  N. Sadeghi,et al.  Primary N2(B) vibrational distributions from excitation-transfer reactions between Kr(3p2) or Xe(3p2) atoms and N2 , 1981 .

[38]  L. G. Piper,et al.  O-Atom Yields from Microwave Discharges in N2O/Ar Mixtures. , 1986 .

[39]  L. G. Piper,et al.  The excitation of IF(B 3Π0+) by N2(A 3Σ+u) , 1985 .