MICROWAVE SPECTRAL TABLES Diatomic Molecules

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$Standard X-ray Diffraction Powder Patterns$

$Standard X-ray Diffraction Powder Patterns$

$Standard X-ray Diffraction$

Nitric oxide1.1508 A————IsotopicMolecularSpeciesJf140 16N150 16Av/pMe/mmVDebye0.158 mB0Mc/sec50848.42m49043.86m%cm-11904eff 2ni/2Mc/sec50121.1548375.04e\'Veff n3/2Mc/sec51571.6149689.35BeMc/sec51109.5149298.14Do.2>2Mc/sec0.0340.017Do.Kn3/2Mc/sec0.3190.261References17391547990011411547, 11411141114111410992IsotopicMolecularSpeciesN140 16N150 16DoMc/sec0.1770.139Q(N)I0-24 cm20.016*oI0^°gcm216.50517.101hlO^W14.41617.019aecm'10.01810.0171Acm'1122.14eqp(N)Mc/sec-2e 2 Q/3 sin 2y\rXJ22 ± 9 Mc/secReferences11411673114111411141154715471547IsotopicMolecularSpeciesK14 0 16N 150 16ReferencesA -doubling, ^-uncouplingconstants, Mc/secPA' P IA-Y a-H76.15 +1.15 +3216.99+170.45 +0.71 +3224.791141magnetic hfs constantsMc/secabed a-(b+c)/283.82 68.49 - 86.34 112.60 92.74-116.94 -96.63 +122.82 -157.88 -130.031547, 114151
IsotopicMolecularSpeciesM14 0 16K15016References, a + (b+c)/2Mc/aec74,8951547— g in Bohr magnetons**2 n+/2 , j = 1/2 2n-/2 , j = 1/2 2 n*/2 , j = 3/2 2 n~/2 , j = 3/2.0007 + a .0007 - a g + (2/5)a g - (2/5)a1041Footnote: ** a = +0.0025, g = -0.0230. For the n3 / 2 state, see 0809, theoreticaltreatment in 1029, and parameters listed here.IsotopicMolecularSpeciesN140 16RotationI nJ *-J3/2+-1/2VibrationVgroundElectronicX/21 -'5/23/2nFlnF3/21/2VMe/sec150176.30 ±0.25150198.52 ±0.25Intensity cm""300° 195°26.E-06 80.E-0698.E-07 29.E-06Ref11413/23/2150218.57 ±0.2578.E-07 24.E-061/21/2150225.47 ±0.2578.E-07 24.E-062 n-/21/21/23/23/2150245.38 ±0.25150375.02 ±0.2598.E-C8 29.E-0798.E-08 29.E-073/23/2150438.72 ±0.2578.E-07 24.E-065/21/23/23/21/21/2150546.25 ±0.25150580.38 ±0.25150644.11 ±0.2526.E-06 80.E-0678.E-07 24.E-0698.E-07 29.E-065/2^3/2groundX/27/25/25/23/2250435.60 ±0.50250439.20 ±0.50ll.E-05 33.E-0572.E-06 21.E-OS11413/21/2250447.16 ±0.5043.F-06 12.F-055Z
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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
Page 22: BrCl Bromine monochloride 2.. Isoto
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Page 27 and 28: IsotopicMolecularSpeciesC3133Br79Cs
Page 29 and 30: IsotopicMolecularSpeciesCS 133F 19R
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Page 45 and 46: IsotopicMolecularSpeciesH2Br81H3Br7
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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
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Page 63 and 64: Inl Indium iodide 2,75-39 AIsotopic
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Page 67 and 68: Lithium iodide 1.3919 AIsotopicMole
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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
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THE NATIONAL BUREAU OF STANDARDSThe
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MICROWAVE SPECTRAL TABLES Diatomic Molecules

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