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Hyperfine Structure of Thallium Bromide

dc.contributor.authorDickinson, J. Thomasen_US
dc.contributor.authorStephenson, David A.en_US
dc.contributor.authorZorn, Jens C.en_US
dc.date.accessioned2010-05-06T22:08:52Z
dc.date.available2010-05-06T22:08:52Z
dc.date.issued1970-08-15en_US
dc.identifier.citationDickinson, J. Thomas; Stephenson, David A.; Zorn, Jens C. (1970). "Hyperfine Structure of Thallium Bromide." The Journal of Chemical Physics 53(4): 1525-1529. <http://hdl.handle.net/2027.42/70429>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70429
dc.description.abstractThe hyperfine structure of the J  =  2J=2 and J  =  3J=3 rotational states of TlBr has been measured with a molecular‐beam electric resonance spectrometer. Hyperfine transition frequencies were measured under conditions of very weak electric and magnetic fields. The linewidth was 500 Hz. The hyperfine interaction constants have been determined for 205Tl79Br, 203Tl79Br, 205Tl81Br, and 203Tl81Br in the first five vibrational states for J  =  2J=2. In addition, the interaction constants for J  =  3,υ  =  0J=3,υ=0 were determined for Tl79Br and Tl81Br, but it was not possible to resolve the effect of the two thallium isotopes in the J  =  3J=3 state. The spectra measured are well described by a hyperfine Hamiltonian containing the bromine quadrupole interaction, the spin–rotation interactions of both the thallium and the bromine nuclei, and both the scalar and tensor parts of the spin–spin interaction between the nuclei. The dependence of the magnetic hfs constants on vibrational state and on isotopic composition shows good agreement with theory. The magnetic octupole interaction of the bromine nucleus in TlBr is negligibly small, and we find no evidence for nuclear polarization or pseudoquadrupole effects.en_US
dc.format.extent3102 bytes
dc.format.extent341467 bytes
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dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleHyperfine Structure of Thallium Bromideen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumRandall Laboratory of Physics, University of Michigan, Ann Arbor, Michigan 48104en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70429/2/JCPSA6-53-4-1525-1.pdf
dc.identifier.doi10.1063/1.1674206en_US
dc.identifier.sourceThe Journal of Chemical Physicsen_US
dc.identifier.citedreferenceG. Gräff, W. Paul, and C. Schlier, Z. Physik 153, 38 (1958); W. Drechsler and G. Gräff, 163, 165 (1961); R. von Boeckh, G. Gräff, and R. Ley, 179, 285 (1964).en_US
dc.identifier.citedreferenceR. H. Hammerle, J. T. Dickinson, R. G. Van Ausdal, D. A. Stephenson, and J. C. Zorn, J. Chem. Phys. 50, 2086 (1969).en_US
dc.identifier.citedreferenceD. A. Stephenson, J. T. Dickinson, and J. C. Zorn, J. Chem. Phys. 53, 1529 (1970), following article.en_US
dc.identifier.citedreferenceA preliminary report of this work has been given: J. T. Dickinson, D. A. Stephenson, and J. C. Zorn, Bull. Am. Phys. Soc. 13, 21 (1968).en_US
dc.identifier.citedreferenceJ. T. Dickinson, Ph.D. thesis, University of Michigan, Ann Arbor, Mich, University Microfilms, Inc., Ann Arbor, Mich., 1968.en_US
dc.identifier.citedreferenceJ. C. Zorn, T. C. English, J. T. Dickinson, and D. A. Stephenson, J. Chem. Phys. 45, 3731 (1966).en_US
dc.identifier.citedreferenceH. G. Fitzky, Z. Physik 151, 351 (1958).en_US
dc.identifier.citedreferenceH. G. Bennewitz, W. Paul, and C. Schlier, Z. Physik 141, 6 (1955).en_US
dc.identifier.citedreferenceA nuclear magnetic octupole interaction has been observed in atomic bromine by H. Brown and J. G. King, Phys. Rev. 142, 53 (1966).en_US
dc.identifier.citedreferenceR. L. White, Rev. Mod. Phys. 27, 276 (1955); C. Schlier, Fortschr. Physik 9, 455 (1961).en_US
dc.identifier.citedreferenceH. J. Zeiger and D. I. Bolef, Phys. Rev. 85, 788 (1952).en_US
dc.identifier.citedreferenceC. H. Townes, “Determination of Nuclear Quadrupole Moments,” in Handbuch der Physik, edited by S. Flügge (Springer, Berlin, 1958), Vol. 38, Pt. 1.en_US
dc.identifier.citedreferenceG. R. Gunther‐Mohr, S. Geschwind, and C. H. Townes, Phys. Rev. 81, 289 (1951); P. A. Bonczyk and V. H. Hughes, 161, 15 (1967).en_US
dc.identifier.citedreferenceH. M. Foley, Phys. Rev. 72, 504 (1947).en_US
dc.identifier.citedreferenceFor TlBr, the ratio of a79/a81a79∕a81 was used for comparison, where a is the first coefficient in Eq. (2). The ratio obtained for TlBr is a79/a81  =  1.1970530(20).a79∕a81=1.1970530(20).en_US
dc.identifier.citedreferenceH. H. Brown and J. G. King, Phys. Rev. 142, 53 (1966). The ratio of quadrupole interaction constants they obtain is b79/b81  =  1.1970568(15).b79∕b81=1.1970568(15).en_US
dc.owningcollnamePhysics, Department of


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