MICROWAVE SPECTRAL TABLES Diatomic Molecules

0898 Mizushima, M. ; Phys. Rev. 94, 569 (1954); Theory of NOthe hyperfine structure of NO molecules.0899 Mizushima, M. ; Phys. Rev. 94, 789 (1954); Theory of NOthe hyperfine structure of NO molecules.0900 Mizushima, M. ; Hill, R. M. , Phys. Rev. 9_3, 745(1954) QZMicrowave spectrum of O .L*0917 Sanders, T. M. , Jr. ; Schawlow, A. L. ; Dousmanis, G. C. ; HOTownes, C. H. ; J. Chem. Phys. 22, 245 (1954); Examinationsof methods for detecting OH.0920 Schneider, E, E. ; Phys. Rev. 9J3» 919 (19 54); Hyperfine LiFstructure in the paramagnetic resonance of X-rayed LiF.0933 Stoicheff, B. P.; Can. J. Phys. _32, 630 (1954); High- NZresolution Raman spectroscopy of gases. III. Ramanspectrum of nitrogen.0938 Tate, P. A. ; Strandberg, M. W. P., J. Chem. Phys. 2,2, NaCl, KC11380 (1954); Stark effect in the microwave spectra of potassiumchloride and sodium chloride.0941 Tinkham, M. ; Strandberg, M. W. P., Phys. Rev. 9J3, O^622 (1954); Selection rules in the microwave magneticresonance spectrum of O .o0944 Trischka, J. W. ; Braunstein, R. , Phys. Rev. 96.' 968 RbCl (MB)(1954); Rotational spectra of RbCl by the molecular beamelectric resonance method.0955 Aamodt, L. C. ; Fletcher, P. C. , Phys. Rev. 98, 1224 COSe, Se(1955); Spin, quadrupole moment, and mass of SE?519550965 Barrett, A. H. ; Mandel, M. , Phys. Rev.