1363 Richardson, J. M. ; Bull. Am. Phys. Soc. 2, 318(1957)Experimental evaluation of the oxygen microwave absorptionas a possible atomic frequency standard.1365 Rosenblum, B. ; Nethercot, A. H. , Jr. ; Bull. Am. Phys.Soc. 2, 44 (1957); Nuclear mass ratios and magnetic effectsin CO71367 Rosenblum, B. ; Nethercot, A. H. , Jr. ; J. Chem. Phys.27, 828 (1957); Quadrupole coupling constant and molecular17structure of CO1368 Russell, A. M. ; Univ. Microfilms, Pub. No. 21928,Dissertation Abstracts 17, 1790 (1957); Rotational magnetic6 ~moments of Li F and Li F.1368 Russell, A. M. ; Phys. Rev. 106, 1100 (1957); Rotational/ 7magnetic moments of Li F and Li F.1370 Schlier, C. ; Z. Physik 147, 600 (1957); Measurement ofthe hyperfine structure of potassium fluoride with the molecular beam resonance method.1383 Stevenson, M. J. ; Bull. Am. Phys. Soc. _2, 31(1957)The quadrupole moment of O1386 Stoicheff, B. P.; Can. J. Phys. 35, 730 (1957); Highresolution Raman spectroscopy of gases. IX. Spectraof H , HD, and D .L* L*1392 Thomas, L. F. ; Heeks, J. S. ; Sheridan, J. ; Arch. Sci.10, 180 (1957); Studies of conjugation and hyper-conjugationin several molecules by microwave spectroscopy.1411 Wilcox, "W. S. ; Southern Research Inst. , Birmingham,Alabama. Final tech. rept. Feb. 27, 1957. Oxygenanalysis by microwave absorption measurements.1414 Zahn, C. T. ; NBS Tech. Rept. - Final Rept., Dec. 31,1957. Microwave absorption of gases.19581425 Barrett, A. H. ; Mandel, M. ; Phys. Rev. 109, 1572(1958); Microwave spectra of the Tl, In, and Ga monohalides.1432 Blaser, J. P. ; Bonanomi, J. ; Nature 182, 859 (1958)Comparison of NH maser with Cs atomic frequencystandard.COCOLiF (MB)LiFKF (AB)co,H 2 (R)Review°2ReviewT1F, T1C1, TIBr,Til, InCl, InBr,Inl, GaCl, GaBr,GalH N, Cs (maser)(AB)139
1434 Boudouris, G. ; Ilias, D. ; Comptes rendues 246, 730 (1958)Microwave absorption of some gaseous solutions.NH + A,NH + CH Cl1435 Boudouris, G 0 ; Ilias, D. ; Comptes rendues 246, 1407 (1958)Measurements of the absorption of microwaves by binarygaseous mixtures.1436 Burrus, C. A. ; J. Chem. Phys. 2S_, 427 (1958); Starkeffect from 1. 1 to 2. 6 mm. wavelength: PH PD , DICO. *1739 Burrus, C. A. ; Graybeal, J. D. ; Phys. Rev. 109, 1553(1958); Stark effect at 2.0 and 1.2 millimeters wavelength:nitric oxide.NH + NH C HO £ £NH C H + AL* L* !DHP, HI, CONO1438 Colpa, J. D. ; Ketelaar, J. A. A. ; Molecular Phys. j_,343 (1958); Pressure-induced rotational absorption spectrumof hydrogen. II,1440 Cowan, M. ; Gordy, W. ; Microwave Lab. , Duke U.Precision measurements of millimeter and submillimeterwave spectra: DC1, DBr, and DI. Aug. 1, 1958.1441 Cowan, M. ; Gordy, W. ; Phys. Rev. Ill, 209 (1958); Precision measurements of millimeter and submillimeter wavespectra: DC1, DBr, DI.1449 Fitzky, H. G. ; Z. Physik 151, 351 (1958); The microwaverotation spectrum of thallium (I) halides.1452 Garrison, A. G. ; Univ. Microfilms, Pub. No. 2732,Dissertation Abstracts 19, 546 (1958); Millimeter wavespectroscopy of molecular beams at high temperature.1454 Graff, G. ; Paul, W. ; Schlier, Ch.; Z. Physik 153, 38(1958); Measurement of the hyperfine structure of T1F bymeans of the molecular-beam-resonance method.HC1, HBr, HIHC1, HBr, HIT1C1, Til, TIBr,T1FReviewT1F (MB)1463 Hurle, I. R. ; Sugden, T. M. ; J. Sci. Instr. 3JJ, 319 CS(1958); Microwave spectrometer for study of free radicals(results presented for CS. )1486 Mizushima, M. ; Phys. Rev. 109, 1557 (1958); Theory of NOthe Stark effect of the NO molecule.1492 Pannetier, G. ; Guenebaut, H. ; Bull. Soc. Chim. France1958, 1463; The rotational structure of the 0, 1 and 1, 0HNbands of the NH radical in the II- S transition.1497 Quinn, W. E. ; Baker, J. M. ; LaTourrette, J. T. ;Rarnsey, N. F. , Jr. ; Phys. Rev. 112, 1929 (1958); Radiofrequencyspectra of hydrogen deuteride in strong magneticfields.H (MB)d*140
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Microwave Spectral TablesVolume I:
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