1498 Ramadier, I. J. ; Amat, G. ; J. Phys. Radium 1^, 915 (1958)Rotational energy of linear molecules. Fourth-order corrections.Review1499 Richardson, J. M. ; J. Appl. Phys. _29, 1 37 (1958); Experimental evaluation of the oxygen microwave absorption asa possible atomic frequency standard,1500 Ring, P. J. ; O'Keefe, J. G. ; Bray, P. J, ; Phys. Rev.7 19Letters _!_, 453 (1958); Li and F nuclear magneticresonances in neutron-irradiated LiF.1501 Rosenblum, B. ; Nethercot, A. H. ; Townes, C. H,Phys. Rev. 109, 400 (1958); Isotopic mass ratios, magnetic moments and the sign of the electric dipole momentin carbon monoxide.1502 Rosenblum, B. ; Townes, C. H. ; Geschwind, S. ; Revs.Mod. Phys. 30, 409 (1958); Recent determinations ofatomic mass ratios by microwave spectroscopy.1503 Russell, A. M. ; Phys. Rev. Ill, 1558 (1958); Magneticmoments due to rotation in Li F and Li F.LiFCOH, C, O, S. Rb,CO, CS, RbClLiF1505 Sessler, A. M. ; Foley, H. M. ; Phys. Rev. 110, 995(1958); Hyperfine structure of deuterium and nucleonnucleonspin-orbit potentials.1506 Sheridan, J. ; Boll. Sci. Fac. Chim. Ind. Bologna 16, 71(1958); Recent progress in the microwave spectroscopy ofgases.Review1511 Tolbert, C. W. ; Douglas, J. H. ; Britt, C. O. ; Tech. Rept.Texas U. Electrical Engineering Research Lab. May 15, 1958Measured absorption of millimeter wavelengths by oxygen atpartial atmospheric pressure.19591529 Burrus, C. A. ; J. Cherru Phys. 30, 976 (1959); Zeemaneffect in the 1- to 3-millimeter wave region: molecular gfactors of several light molecules.HBr, CO, HI,CL1530 Burrus, C. A. ; J. Chem. Phys. 31, 1270 (1959); Starkeffect at 0.93, 1. 18, and 1. 5 millimeters wavelength; DC1,DBr, and DLHC1, HBr, HI1534 Colpa-Boonstra, J. P. ; France Centre Natl. RecherchesSci. 77, 41 (1959); Rotational spectra of pure molecularhydrogen induced by pressure.141
1547 Favero, P. G. ; Mirri, A. M. ; Gora . , W. ; Duke U. NOMicrowave Lab. (1959); Millimeter- wave rotational spectrumof NO in the 7T/ state.1558 Iddings, C. K. ; Platzman, P. M. ; Phys. Rev. 113, 192 H Z(1959); Nuclear structure correction to the hyperfine structurein hydrogen.1559 Iddings, C. K. ; Platzman, P. M. ; Phys. Rev. 115, 919 H(1959); Meson corrections to the hyperfine structure inhydrogen.1587 Maryott, A. A. ; Kryder, S. J. ; J. Chem, Phys. 31, NO617 (1959); Nonresonant microwave absorption and electric dipole moment of NO in the gaseous state.1591 Mizushima, M. ; Tech. Rept. - Colorado University, OJan. — Mar. 1959. Research studies in connection withmicrowave spectrum of the O molecule.1599 Pannetier, G. ; Guenebaut, H. ; Hajal, I. ; Bull. Soc. Chim. HNFrance 1959, 1159; Rotational analysis of the (O, O) bandof the II - S transition of the ND radical.1605 Ransil, B. J. ; J. Chem. Phys. ^30, 1 1 13 (1959); Quadrupole COcoupling constant, dipole moment, and electron populationof CO.I9601641 Cowan, M. J. ; Univ. Microfilms, Pub. No. 26Z, Disser- HI, HC1, HBr, COtation Abstracts 20, 4139 (I960); Microwave spectroscopyin the 0. 5 to 1.5 millimeter wave region: HI, DC1, DBr,DI, and CO.1654 James, T. C. ; Norris, W. G. ; Klemperer, W. ; J. Chem. LiH (IR)Phys. 32, 728 (I960); Infrared spectrum and dipole momentfunction of lithium hydride.1667 Lefebvre-Brion, H. ; Moser, C. M. ; Phys. Rev. 118, 675 NO(I960); Calculation of the magnetic hyperfine structure couplingconstants of NO.1673 Lin, C. C. ; Phys. Rev. 119, 1027 (I960); Hyperfine structure NOof the microwave spectra of the NO molecule and the nuclearquadrupole moment of nitrogen.1674 Lin, C. C. ; Hijikata, K. ; Sakamoto, M. ; Oklahoma U. NOResearch Institute (I960); Electronic structure and hyperfine structure constants of NO molecule.1682 Maryott, A. A. ; Birnbaum, G. ; J. Chem. Phys. 32, 686 O(I960); Microwave absorption in compressed oxygen.142
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Microwave Spectral TablesVolume I:
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Casimir's function and the hyperfin
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