Calibration lines of HCN in the 1.5-microm region.

Near-IR distributed feedback semiconductor laser spectroscopy of HCN in natural abundance and in an H(13)CN-enriched sample has been performed from 6380 to 6410 cm(-1). Absolute accuracy of wavenumber measurement was 0.0005 cm(-1) using the 3-0 band of CO as a reference. New sets of molecular constants for the (2 0(0) 0)-(0 0(0) 0) and (2 1(1) 0)-(0 1(1) 0) bands of H(12)C(14)N and H(13)C(14)N have been determined by combining the present results together with the existing data. Two tables of the calculated wavenumbers are given for calibration standards in the 1.5-microm region.

[1]  T. A. Wiggins,et al.  Secondary and Tertiary Interferometric Wavelength Standards in the 1.5–2.5 μ Region* , 1957 .

[2]  Tsutomu Yanagawa,et al.  Frequency stabilization of 1.5‐μm InGaAsP distributed feedback laser to NH3 absorption lines , 1984 .

[3]  H. Sasada,et al.  1.5-μm DFB semiconductor laser spectroscopy of deuterated water , 1989 .

[4]  K. Lehmann,et al.  Fourier transform spectra of overtone bands of HCN from 5400 to 15100 cm−1 , 1989 .

[5]  Yoshio Noguchi,et al.  Frequency stabilization of an InGaAsP distributed feedback laser to an NH3 absorption line at 15137 Å with an external frequency modulator , 1985 .

[6]  Robert A. Toth,et al.  Comparison of the frequencies of NH 3 , CO 2 , H 2 O, N 2 O, CO, and CH 4 as infrared calibration standards , 1985 .

[7]  N. Ohashi,et al.  1.3-μm DFB diode laser spectroscopy of 12C2H2 , 1989 .

[8]  H. Foley Self-Broadening in the 14 μ Band of HCN , 1946 .

[9]  Donald E. Jennings,et al.  The ground state of molecular hydrogen , 1983 .

[10]  L. Yarmus Hyperfine Structure in thel-Type Doubling Spectrum of HCN , 1956 .

[11]  T. Törring l-Typ-Dubletts der isotopen HCN-Molekeln , 1961 .

[12]  K. Evenson,et al.  Heterodyne frequency measurements of 12C16O laser transitions , 1989 .

[13]  C. Burrus,et al.  Millimeter and Submillimeter Wave Spectroscopy , 1956 .

[14]  K. Lehmann,et al.  The intensity and self‐broadening of overtone transitions in HCN , 1986 .

[15]  F. Delucia,et al.  Molecular-Beam Maser for the Shorter-Millimeter-Wave Region: Spectral Constants of HCN and DCN , 1969 .

[16]  D. Lide,et al.  Microwave and Infrared Measurements on HCN and DCN: Observations on l‐Type Resonance Doublets , 1967 .

[17]  G. Winnewisser,et al.  ROTATIONAL CONSTANTS FOR HCN AND DCN. , 1971 .

[18]  H. Sasada 1.5 μm DFB semiconductor laser spectroscopy of HCN , 1988 .

[19]  G. Winnewisser,et al.  The Molecular Structures of HNC and HCN Derived from the Eight Stable Isotopic Species , 1976 .

[20]  Jean-Pierre Bouanich,et al.  Étalonnage et déplacement des raies de vibration-rotation des bandes 0 → 2 et 0 → 3 de l'oxyde de carbone , 1974 .

[21]  Guy Guelachvili,et al.  Dunham coefficients for seven isotopic species of CO , 1983 .

[22]  A. G. Maki,et al.  Absolute frequency measurements of the 2-0 band of CO at 2.3 μm; Calibration standard frequencies from high resolution color center laser spectroscopy , 1983 .

[23]  S. Kinugawa,et al.  Wavenumber Measurement of the 1.5-µm Band of Acetylene by Semiconductor Laser Spectrometer , 1990 .

[24]  K. Evenson,et al.  Frequency measurement of the 260-THz (1.15-microm) He-Ne laser. , 1979, Optics letters.

[25]  H. Sasada,et al.  Observation of the 2ν1 band of HN+2 with a 1.57 μm distributed feedback semiconductor laser , 1990 .