Submillimeter-wave spectroscopy of VN (X3Δr) and VO (X4Σ−): A study of the hyperfine interactions

[1]  Hajime Yano,et al.  Mineralogy and Petrology of Comet 81P/Wild 2 Nucleus Samples , 2006, Science.

[2]  L. Ziurys,et al.  Velocity modulation spectroscopy of molecular ions I: The pure rotational spectrum of TiCl+ (X3Φr) , 2005 .

[3]  L. Ziurys,et al.  A millimeter/submillimeter velocity modulation spectrometer for studies of molecular ions , 2005 .

[4]  M. Kaasik,et al.  Trace Metals in Mosses in the Estonian Oil Shale Processing Region , 2004 .

[5]  A. J. Merer,et al.  Laser spectroscopy of VS: hyperfine and rotational structure of the C4Σ−–X4Σ− transition , 2003 .

[6]  R. S. Ram,et al.  Infrared emission spectroscopy and ab initio calculations on VCl , 2003 .

[7]  R. S. Ram,et al.  NoteFourier Transform Emission Spectroscopy of the f1Φ–a1Δ System of VN , 2002 .

[8]  R. S. Ram,et al.  Infrared emission spectroscopy of the [10.5]5Δ-X5Δ system of VF , 2002 .

[9]  R. S. Ram,et al.  Fourier Transform Emission Spectroscopy of a New 2Φ–12Δ System of VO , 2002 .

[10]  R. S. Ram,et al.  Emission Spectroscopy of the d1Σ+–b1Σ+, d1Σ+–X3Δ1, and e1Π–a1Δ Systems of VN , 2001 .

[11]  R. S. Ram,et al.  Fourier transform infrared emission spectroscopy of VCl , 2001 .

[12]  The pure rotational spectra of TiO(X3Δ) and TiN(X2Σ , 1998 .

[13]  A. J. Merer,et al.  Rotational and Hyperfine Structure in the B4Π-X4Σ− (0,0) Band of VO at 7900 Å: Perturbations by the a2Σ+, v = 2 Level , 1995 .

[14]  A. J. Merer,et al.  Laser-Induced Fluorescence of Gaseous Vanadium Methylidyne, VCH: A Triatomic Organometallic Molecule , 1995 .

[15]  A. J. Merer,et al.  Hyperfine structure in high spin multiplicity electronic states: Analysis of the B 4Π–X 4Σ− transition of gaseous NbO , 1994 .

[16]  A. J. Merer,et al.  Rotational, fine, and hyperfine analyses of the (0,0) band of the D 3Π–X 3Δ system of vanadium mononitride , 1993 .

[17]  A. J. Merer,et al.  Elucidation of electronic structure by the analysis of hyperfine interactions: The MnH A 7Π–X 7Σ+ (0,0) band , 1991 .

[18]  G. T. Fraser,et al.  Microwave spectra and electric dipole moments of X4Σ12−1 VO and NbO , 1991 .

[19]  J. Brett.  Astrophysical oscillator strengths for TiO and VO bands from spectrum synthesis of spectral types M1 III to M7 III , 1990 .

[20]  B. Simard,et al.  Spectroscopy and photophysics of refractory molecules at low temperature: The d1Σ+-X3Δ1 intercombination system of vanadium nitride , 1989 .

[21]  A. J. Merer,et al.  Spin–orbit distortion of the hyperfine structure in heavier molecules: Breakdown of the case (aβ) formalism in the B 3Φ–X 3Δ system of gaseous NbN , 1989 .

[22]  A. J. Merer,et al.  Fourier transform spectroscopy of VO: Rotational structure in the A4Π-X4Σ− system near 10 500 Å , 1982 .

[23]  A. J. Merer,et al.  Laser spectroscopy of VO: Analysis of the rotational and hyperfine structure of the C4Σ−-X4Σ− (0, 0) band , 1982 .

[24]  W. J. Childs,et al.  Laser-rf double-resonance studies of the hyperfine structure of /sup 51/V , 1979 .

[25]  R. F. Barrow,et al.  New Type of Perturbation caused by a Magnetic Hyperfine Interaction, observed in the Ground State of VO , 1968 .