The Schumann-Runge absorption bands of 16O18O in the wavelength region 175–205 nm and spectroscopic constants of isotopic oxygen molecules

[1]  D. E. Freeman,et al.  Wavelength measurement and analysis of the Schumann-Runge absorption bands of 18O2 in the region 175–205 nm , 1988 .

[2]  J. R. Esmond,et al.  High resolution absorption cross-sections and band oscillator strengths of the Schumann-Runge bands of oxygen at 79 K , 1987 .

[3]  J. Frederick,et al.  Atmospheric odd oxygen production due to the photodissociation of ordinary and isotopic molecular oxygen , 1987 .

[4]  B. Lewis,et al.  Predissociation linewidths for the Schumann-Runge bands of 16O18O , 1987 .

[5]  R. Field,et al.  Reinvestigation of the CO A1Π state and its perturbations: The v = 0 level , 1987 .

[6]  D. E. Freeman,et al.  Molecular spectroscopic constants of O2(B3Σu−): The upper state of the Schumann-Runge bands , 1986 .

[7]  S. Gibson,et al.  Decomposition of the photoabsorption continuum underlying the Schumann-Runge bands of 16O2—I. Role of the B 3Σu- state: A new dissociation limit , 1985 .

[8]  S. Gibson,et al.  Photodissociation of 16O18O in the atmosphere , 1984 .

[9]  K. Yoshino,et al.  High resolution absorption cross section measurements and band oscillator strengths of the (1,0)-(12,0) Schumann-Runge bands of O2 , 1983 .

[10]  R. Cicerone,et al.  Photodissociation of isotopically heavy O 2 as a source of atmospheric O 3 , 1980 .

[11]  E. Colbourn,et al.  An effective Hamiltonian for diatomic molecules . Ab initio calculations of parameters of HCl , 1979 .

[12]  Bowen Liu,et al.  Abinitio configuration interaction study of the valence states of O2 , 1977 .

[13]  A. Bandrauk,et al.  Predissociation linewidths and level shifts for double‐curve crossing models , 1977 .

[14]  J. Watson,et al.  Spin-orbit and spin-rotation coupling in doublet states of diatomic molecules , 1977 .

[15]  P. Julienne.  3Σu−-3Σu+ coupling in the O2 B3Σu− predissociation☆ , 1976 .

[16]  J. Brown,et al.  Spin-dependent interactions for linear molecules in Σ states of quartet and higher multiplicity , 1976 .

[17]  W. Stwalley.  Mass‐reduced quantum numbers: Application to the isotopic mercury hydrides , 1975 .

[18]  W. Gordy,et al.  Microwave spectrum and molecular constants ofO16O18 , 1975 .

[19]  M. Krauss,et al.  Predissociation of the Schumann-Runge bands of O2 , 1974 .

[20]  J. C. Baird,et al.  Spin—Orbit Effects and the Fine Structure in the 3Σg− Ground State of O2 , 1967 .

[21]  M. Halmann,et al.  Isotope Effects on Vibrational Transition Probabilities. II. Electronic Transitions of Isotopic Nitrogen, Nitric Oxide, and Oxygen Molecules , 1965 .

[22]  M. Tinkham.  Theory of the fine structure of the molecular oxygen ground state with an experimental study of its microwave paramagnetic spectrum , 1955 .

[23]  G. Herzberg,et al.  FINE STRUCTURE OF THE SCHUMANN-RUNGE BANDS NEAR THE CONVERGENCE LIMIT AND THE DISSOCIATION ENERGY OF THE OXYGEN MOLECULE , 1954 .

[24]  D. R. Bates.  Suggested explanation of heavy ozone , 1988 .

[25]  Konrad Mauersberger,et al.  Ozone isotope measurements in the stratosphere , 1987 .

[26]  D. E. Freeman,et al.  Atlas of the Schumann–Runge Absorption Bands of O2 in the Wavelength Region 175–205 nm , 1984 .

[27]  D. E. Freeman,et al.  Photoelectric scanning (6.65-m) spectrometer for VUV cross-section measurements. , 1980, Applied optics.

[28]  I. Laulicht,et al.  Isotope Effects on Vibrational Transition Probabilities. The Schumann—Runge Absorption Bands of 16O2 and 18O2 , 1965 .