MICROWAVE SPECTRAL TABLES Diatomic Molecules

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$Standard X-ray Diffraction Powder Patterns$

$Standard X-ray Diffraction Powder Patterns$

$Standard X-ray Diffraction$

IsotopicMolecularSpeciesGa71Cl35Rotationt «J «-J2
IsotopicMolecularSpeciesGa71Cl37RotationjVj"2«-lVibrationVground'I7/27/27/27/27/27/25/25/2?/25/25/2F'54332243211itpi5/25/25/25/25/25/23/23/23/23/23/2nF43322133110VMe/ sec17118.24 ±0.5017118.24 ±0.5017118.24 ±0.5017118.24 ±0.5017118.24 ±0.5017118.24 ±0.5017118.24 ±0.5017118.24 ±0.5017118.24 ±0.5017118.24 ±0.5017118.24 ±0.50total intensityIntensity cm""300° 195°13.E~08R38.E-0893.E-09R28.E-0814.E-09R43.E-0966.E-09R20.E-0811.E-09R33.E-0946.E-09R14.E-0873.E-09R22.E-08ll.E-09R34.E-0925.E-09R76.E-0911.E-09R32.E-0912.E-09R36.E-0949.E-08R15.E-07Ref1425Gal Gallium monoiodide 2.5747 A©-----©IsotopicMolecularSpeciesGa69 x127to71!127ReferencesAv/pMe/mmM-DebyeBeMe/sec1706.86 m1675.73 m1425wecm"12169900eqQ(I)Me/sec-5491425eqQ(Ga)Me/sec-661425aeMe/ sec5.6675.5351425Dekc/sec0.471425AdditionalMicrowaveReferences1192, 1341Footnote: Intensities for those components of degenerate lines were not computed if they involvedforbidden transitions, in this case , AF^ = 3.22
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Page 5 and 6: Microwave Spectral TablesVolume I:
Page 7 and 8: Casimir's function and the hyperfin
Page 9 and 10: axis, II indicates the II electroni
Page 14 and 15: Z = the sum of the Boltzmann factor
Page 17 and 18: (11)J««-J transition,F^ ; i.j.r)s
Page 22: BrCl Bromine monochloride 2.. Isoto
Page 25 and 26: IsotopicMolecularSpeciesC 12 S33C 1
Page 27 and 28: IsotopicMolecularSpeciesC3133Br79Cs
Page 29 and 30: IsotopicMolecularSpeciesCS 133F 19R
Page 31 and 32: CDinCMrHrH CO(Tj d> CUCJ > 0o KJ G-
Page 33 and 34: IsotopicMolecularSpeciesGa69Br79Ga6
Page 35 and 36: IsotopicMolecularSpeciesGa71Br79Rot
Page 37 and 38: IsotopicMolecularSpeciesGa69 Cl35Ro
Page 39: TsotopicMolecularSpeciesGa69 Cl35Ro
Page 43 and 44: IsotopicMolecularSpeciesto69 !127Ro
Page 45 and 46: IsotopicMolecularSpeciesH2Br81H3Br7
Page 47 and 48: IsotopicMolecularSpeciesH2 !127H3 !
Page 49 and 50: Since V depends only upon the coupl
Page 51 and 52: IsotopicMolecularSpeciesHV 6H20 16R
Page 53 and 54: InBrIndium bromide(L.}-----Isotopic
Page 55 and 56: IsotopicMolecularSpeciesIn115Br79Ro
Page 57 and 58: IsotopicMolecularSpeciesIn 115Br79R
Page 59 and 60: IsotopicMolecularSpeciesIn 115Br79R
Page 61 and 62: IsotopicMolecularSpeciesIn 115Cl35R
Page 63 and 64: Inl Indium iodide 2,75-39 AIsotopic
Page 65 and 66: IsotopicMolecularSpecies1^38Rotat i
Page 67 and 68: Lithium iodide 1.3919 AIsotopicMole
Page 69 and 70: Hence, the approximationwas used.Si
Page 71 and 72: IsotopicMolecularSpeciesM14 0 16K15
Page 73 and 74: 0 2 Oxygen3 —The ground electroni
Page 75 and 76: Oxygen 1.2074 1--©IsotopicMolecula
Page 77 and 78: IsotopicMolecularSpecieso216° 2180
Page 79 and 80: TsotopicMolecularSpecies0 160 18Rot
Page 81 and 82: Iso topicMolecularSpeciesK^Br79K^Br
Page 83 and 84: IsotopicMolecularSpeciesK^Cl35Rotat
Page 85 and 86: IsotopicMolecularSpeciesK^Cl36Rotat
Page 87 and 88: IsotopicMolecularSpeciesRb85Br79Rot
Page 89 and 90: IsotopicMolecularSpeciesRb85Cl35Rot
Page 91 and 92:
IsotopicMolecularSpecieslfa23Br79Ro
Page 93 and 94:
laotopicMolecularSpeciesSa23Cl37Ref
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IsotopicMolecularSpecies«a23I127Ro
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IsotopicMolecularSpeciesTl205Br79Ro
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IsotopicMolecularSpeciesTl205Br81Ro
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IsotopicMolecularSpeciesT1203C135Ro
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IsotopicMolecularSpeciesT1 2Q5F19Ro
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IsotopicMolecularSpeciesT1205 ][ 12
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19330004 Wick, G. C. , Z. Physik 85
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0190 Gilbert, D. A. ; Roberts, A. ;
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0375 Woodward, Nature 165, 198 (195
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0518 Carls on, R. O. ; Lee, C. A. ;
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0722 Lee, C. A. ; Fabric and, B. P.
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0898 Mizushima, M. ; Phys. Rev. 94,
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1061 Rosenblum, B. ; Nethercot, A.
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1235 Solomon, I. ; Bloembergen, N,
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1434 Boudouris, G. ; Ilias, D. ; Co
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1547 Favero, P. G. ; Mirri, A. M. ;
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9900 American Institute of Physics
Page 165:
THE NATIONAL BUREAU OF STANDARDSThe
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MICROWAVE SPECTRAL TABLES Diatomic Molecules

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