0622 Swartz, J. C. ; Trischka, J. W. , Phys. Rev. 88, 10856 19(1952); Radiofrequency spectra of Li F by the molecularbeamelectric-resonance method.0628 Trischka, J. W. ; J. Chem. Phys. 2Q_, 1811 (1952); On theinternuclear distance and dipole moment of the LiF molecule.LiF (MB)LiF0637 Wieland, K. ; Waser, J. , Phys. Rev. 8J3, 385 (1952); Themolecular spectrum of iodine excited in the presence of aninert gas.19530649 Arnowitt, R. ; Phys. Rev. 92, 1002 (1953); The hyperfinestructure of hydrogen.1732 Altshuller, A. P. ; J. Chem. Phys. 2J_, 2074(1953)Dipole moments of gaseous thallous halides.0650 Artman, J. O. ; Gordon, J. P. , Phys. Rev. 20, 338(1953); Pressure broadening of oxygen lines in the millimeter wave-length region.0654 Bates, D. R. ; Poots, F. , Proc. Phys. Soc. 66A, 784(1953); Properties of the hydrogen molecular ion. I.Quadrupole transitions in the ground electronic state anddipole transitions of the isotopic ions.0671 Burrus, C. A. ; Gordy, W. , Phys. Rev. 92_, 1437(1953)One-to-two millimeter wave spectroscopy III. NO and DI.H, H ZTIBr, Til4NO, HI0679 Dieke, G. H. ; Cunningham, S. P. ; Byrne, F. T. , Phys.Rev. 92, 81 (1953); The Zeeman effect in the molecularspectra of hydrogen.H ,Zeeman0684 Fabricand, B. P. ; Carlson, R. O. ; Lee, C. A, ; Rabi, I. I.Phys. Rev. 9_1, 1403 (1953); The rotational levels of KBrand their hyperfine structure.0693 Harrick, N. J. ; Barnes, R. B.; Bray, P. J. ;Ramsey, N. F. , Jr. ; Phys. Rev. 90, 260 (1953); Nuclearradiofrequency spectra of D and H in intermediate andstrong magnetic fields.0699 Honig, A. ; Stitch, M. L. ; Mandel, M. , Phys. Rev. 92,901, (1953); Microwave spectra of CsF, CsCl, CsBr.0716 Klein, J. A. ; Nether cot, A. H. , Jr., Phys. Rev. 90.*1018 (1953); Microwave spectrum of DI and 1. 5 mm.wavelength.0721 Kusch, P. ; Phys. Rev. 92, 268 (1953); Sign of quadrupoleinteraction.KBr (MB)H 0 (MB)CsF, CsCl, CsBrHILiCl (MB)131
0722 Lee, C. A. ; Fabric and, B. P.; Carlson, R. O.jRabi, I. I. , KC1 (MB)Phys. Rev. 91, 1395 (1953); Molecular-beam investigationof rotational transitions. I, The rotational levels of KC1and their hyperfine structures.0736 Miller, S. L. ; Univ. Microfilms, Pub. No. 4585, Disserta- Otion Abstracts 13, 110 (1953); The microwave absorptionspectrum of oxygen,0737 Miller, S. L. ; Townes, C. H. , Phys. Rev. 9£, 537(1953) Q ZThe microwave absorption spectrum of O and O Oz0738 Miller, S. ; Townes, C. H. ; Kotani, M. , Phys. Rev. 90, O542 (1953)0741 Mizushima, M. ; Phys. Rev. £1, 222 (1953); On the frequen- QZcies of the microwave absorption lines of oxygen.0752 Poots, G. ; Proc. Phys. Soc. 66A, 1181 (1953); The effect QZof variation of the dipole moment with internuclear separationon the relative intensities of the second negative band systemof oxygen.0757 Ramsey, N. F. , Jr., Phys. Rev. 89^, 527 (1953); Psuedo- H^quadrupole effect for nuclei in molecules.0758 Ramsey, N. F. , Jr. ; Science 1 \1_, 470 (1953); Electron HZ (MB)distribution in molecular hydrogen.0764 Sanders, T. M. ; Schawlow, A. L. ; Dousmanis, G. C. ; OHTownes, C. H. ; Phys. Rev. 89, 1158 (1953); A microwave spectrum of the free OH radical.0775 Tate, P. ; Strandberg, M. W. P. , Phys. Rev. 9_1_, 464 KC1, NaCl(1953); Stark effect in high temperature microwave spectroscopy.0792 Wimett, T. F. ; Phys. Rev. 9J., 476 (1953); Nuclear H Zresonance line structure in HD and molecular shieldingin HD, H , and D .0793 Wolfsberg, M. ; J. Chem. Phys. 2j_, 2166 (1953); Note on N Za nitrogen molecule calculation.19540797 Artman, J. O. ; Gordon, J. P. , Phys. Rev. 96, 1237 O(1954); Absorption of microwaves by oxygen in the millimeter wave-length.0803 Barnes, R. G. ; Bray, P. J. ; Ramsey, N. F. , Jr., Phys. HRev - 94, 893 (1954); Variations of hydrogen rotationalmagnetic moments with rotational quantum number andwith isotopic mass.132
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Microwave Spectral TablesVolume I:
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Casimir's function and the hyperfin
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(11)J««-J transition,F^ ; i.j.r)s
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BrCl Bromine monochloride 2.. Isoto
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