D. G. S. Snyder
National Oceanic and Atmospheric Administration
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Featured researches published by D. G. S. Snyder.
Journal of Molecular Spectroscopy | 1982
V. Malathy Devi; B. Fridovich; G. D. Jones; D. G. S. Snyder; Palash P. Das; J.-M. Flaud; C. Camy-Peyret; K. Narahari Rao
Abstract High-resolution spectra in the ν 3 region of 14 N 16 O 2 were measured by using a diode laser as a source to a vacuum grating spectrometer. Spin-rotation constants for the ν 3 and ν 2 + ν 3 states were determined from the observed data. Absolute strengths and transition moments for the ν 3 and ν 2 + ν 3 − ν 2 bands were derived from the observed line strengths at 296 K. Self-broadened and N 2 -broadened half-widths were measured for several of the ν 3 band lines at room temperature. Temperature-dependent half-widths for two N 2 -broadened ν 3 lines are also reported.
Journal of Molecular Spectroscopy | 1984
V. Malathy Devi; B. Fridovich; G. D. Jones; D. G. S. Snyder
Abstract Absolute line strengths have been measured at room temperature for spectral lines in the R branch of the ν3 band of 12C16O2, 12C16O18O, and 12C16O17O and the (ν2 + ν3) − ν2 and (ν1 + ν3) − ν1 bands of 12C16O2 in the region 2365–2393 cm−1 using a tunable diode laser spectrometer; from these measurements band strengths have been computed. Self- and nitrogen-broadened half-widths have been measured for some ν3 lines of 12C16O2 and 12C16O17O, and nitrogen-broadened half-widths measured for some (ν2 + ν3) − ν2 band lines of 12C16O2. From measurements made over a temperature range from 217 to 299 K we have obtained temperature coefficients n, for the N2-broadened Lorentz half-width defined as b L 0 (T) = b L 0 (T 0 )( T T 0 ) −n , for the ν3 and (ν2 + ν3) − ν2 bands of 12C16O2. They are 0.757 ± 0.008 and 0.789 ± 0.015, respectively.
Journal of Molecular Spectroscopy | 1983
V. Malathy Devi; B. Fridovich; G. D. Jones; D. G. S. Snyder
Abstract Line strengths and self- and nitrogen-broadened half-widths were measured for spectral lines in the ν3 and ν2 + ν4 bands of 12CH4 and 13CH4 from 2870–2883 cm−1 using a tunable diode laser spectrometer. From measurements made over a temperature range from 215 to 297 K, on samples of 12CH4 broadened with N2, we deduced that the average temperature coefficients n, defined as b L 0 (T) = b L 0 (T 0 )( T T 0 ) −n , of the Lorentz broadening coefficients for the ν3 and ν2 + ν4 bands of 12CH4 were 0.97 ± 0.03 and 0.89 ± 0.04, respectively. A smaller increase is observed in line half-width with increasing pressure for E-species lines, for both self- and nitrogen-broadening, than for other symmetry species lines over the range of pressures measured, 70 to 100 Torr.
Journal of Quantitative Spectroscopy & Radiative Transfer | 1983
V. Malathy Devi; B. Fridovich; D. G. S. Snyder; G. D. Jones; Palash P. Das
Abstract Absolute line strengths and self-, nitrogen-, and air-broadened half-widths, for five lines in the R -branch of the ν 2 fundamental of methane have been measured at room temperature using a tunable diode laser spectrometer.
Journal of Molecular Spectroscopy | 1985
V. Malathy Devi; B. Fridovich; G. D. Jones; D. G. S. Snyder
Abstract Intensities and half-widths have been measured, using a tunable diode laser, for several water vapor lines in the ν 2 spectral region between 1500 and 1523 cm −1 . Where possible, results have been compared with previously published values.
Journal of Geophysical Research | 1984
C. P. Rinsland; A. Goldman; V. Malathy Devi; B. Fridovich; D. G. S. Snyder; G. D. Jones; F. J. Murcray; D. G. Murcray; M. A. H. Smith; R. K. Seals; M. T. Coffey; William G. Mankin
Applied Optics | 1982
V. Malathy Devi; B. Fridovich; G. D. Jones; D. G. S. Snyder; A. Neuendorffer
Archive | 1983
K. Narahari Rao; V. Malathy Devi; B. Fridovich; D. G. S. Snyder; G. D. Jones
Archive | 1983
V. Malathy Devi; B. Fridovich; D. J. Jones; D. G. S. Snyder
Journal of Molecular Spectroscopy | 1983
V. Malathy Devi; B. Fridovich; G. D. Jones; D. G. S. Snyder