MICROWAVE SPECTRAL TABLES Diatomic Molecules

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$Standard X-ray Diffraction Powder Patterns$

$Standard X-ray Diffraction Powder Patterns$

$Standard X-ray Diffraction$

BibliographyThe references are listed in numerical order. Numbers below1725 are assigned according to year and then alphabeticallyaccording to the first author. References added after the initialnumbering are listed according to both numerical and yearauthororders.
19330004 Wick, G. C. , Z. Physik 85, 25 (1933); Magnetic momentof a rotating hydrogen molecule.H19370010 Schlapp, R. , Phys. Rev. 51, 342 (1937); Fine structureO rotationin the 2 ground state of C^, and the rotational intensitydistribution in the atmospheric oxygen band.19390015 Hamilton, D. R. , Phys. Rev. 56, 30 (1939); Hyperfine2 115metastable PS/2 state of In I and electric quadrupoleIln (AB)moment of In0016 Kellogg, J. M. B. ; Rabi, I. I. ; Ramsey, N. F. , Jr.;Zacharias, J. R. , Phys. Rev. _55, 318 (1939); Anelectrical quadrupole moment of the deuteron.(MB)0017 Kellogg, J. M. B. ; Rabi, I. I. ; Ramsey, N. F. , Jr.;Zacharias, J. R. , Phys. Rev. 56, 728 (1939)- Magneticmoments of proton and deuteron. Radiofrequency spectraof H in magnetic fields.H (MB)19400022 Kellogg, J. M. B. ; Rabi, I. I. ; Ramsey, N. F. , Jr. ;Zacharias, J. R. , Phys. Rev. 57, 677 (1940); Electricalquadrupole moment of deuteron. Radiofrequency spectraof HD and D molecules in magnetic field.LJH (MB)Li0028 Ramsey, N. F. Phys. Rev. 58, 226 (1940); Rotationalmagnetic moments of H , D and HD molecules. Rotational radiofrequency spectra of H , D and HD inmagnetic fields.0030 Scheffers, H. , Phys. Zeits. 41, 89 (1940); Determinationof dipole moments by molecular ray method.HC1 (MB)19410031 Brooks, H. , Phys. Rev. 60, 168 (1941); Interactionbetween nuclear spin and molecular rotation.H hype rfine19451744 Van Vleck, J. H. , Report 664 from Radiation LaboratoryMIT (March 1, 1945); Further theoretical investigations onthe atmospheric absorption of microwaves.H 2°> °219460036 Beringer, R. , Phys. Rev. 70, 53 (1946); Absorption of 0. 5cm. waves in O .L*C)124
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UNITED STATES DEPARTMENT OF COMMERC
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Microwave Spectral TablesVolume I:
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Casimir's function and the hyperfin
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axis, II indicates the II electroni
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Z = the sum of the Boltzmann factor
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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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IsotopicMolecularSpeciesC 12 S33C 1
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IsotopicMolecularSpeciesC3133Br79Cs
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IsotopicMolecularSpeciesCS 133F 19R
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CDinCMrHrH CO(Tj d> CUCJ > 0o KJ G-
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IsotopicMolecularSpeciesGa69Br79Ga6
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IsotopicMolecularSpeciesGa71Br79Rot
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IsotopicMolecularSpeciesGa69 Cl35Ro
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TsotopicMolecularSpeciesGa69 Cl35Ro
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IsotopicMolecularSpeciesGa71Cl37Rot
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IsotopicMolecularSpeciesto69 !127Ro
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IsotopicMolecularSpeciesH2Br81H3Br7
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IsotopicMolecularSpeciesH2 !127H3 !
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Since V depends only upon the coupl
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IsotopicMolecularSpeciesHV 6H20 16R
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InBrIndium bromide(L.}-----Isotopic
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IsotopicMolecularSpeciesIn115Br79Ro
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IsotopicMolecularSpeciesIn 115Br79R
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IsotopicMolecularSpeciesIn 115Br79R
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IsotopicMolecularSpeciesIn 115Cl35R
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Inl Indium iodide 2,75-39 AIsotopic
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IsotopicMolecularSpecies1^38Rotat i
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Lithium iodide 1.3919 AIsotopicMole
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Hence, the approximationwas used.Si
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IsotopicMolecularSpeciesM14 0 16K15
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0 2 Oxygen3 —The ground electroni
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Oxygen 1.2074 1--©IsotopicMolecula
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IsotopicMolecularSpecieso216° 2180
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TsotopicMolecularSpecies0 160 18Rot
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Iso topicMolecularSpeciesK^Br79K^Br
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IsotopicMolecularSpeciesK^Cl35Rotat
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IsotopicMolecularSpeciesK^Cl36Rotat
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IsotopicMolecularSpeciesRb85Br79Rot
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IsotopicMolecularSpeciesRb85Cl35Rot
Page 91 and 92: IsotopicMolecularSpecieslfa23Br79Ro
Page 93 and 94: laotopicMolecularSpeciesSa23Cl37Ref
Page 95 and 96: IsotopicMolecularSpecies«a23I127Ro
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Page 103 and 104: IsotopicMolecularSpeciesT1 2Q5F19Ro
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MICROWAVE SPECTRAL TABLES Diatomic Molecules

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