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Electron diffraction studies of hot molecules. II. ‘‘Anharmonic shrinkage effects’’ in SF6, CF4, and SiF4

dc.contributor.authorGoates, Steven R.en_US
dc.contributor.authorBartell, Lawrence S.en_US
dc.date.accessioned2010-05-06T22:27:17Z
dc.date.available2010-05-06T22:27:17Z
dc.date.issued1982-08-15en_US
dc.identifier.citationGoates, Steven R.; Bartell, Lawrence S. (1982). "Electron diffraction studies of hot molecules. II. ‘‘Anharmonic shrinkage effects’’ in SF6, CF4, and SiF4." The Journal of Chemical Physics 77(4): 1874-1877. <http://hdl.handle.net/2027.42/70624>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70624
dc.description.abstractLeast squares refinements of diffraction intensities for SF6, CF4, and SiF4 yielded nonbonded internuclear distances that lagged increasingly behind values expected from the bond lengths, the higher the temperature. The observation that observed nonbonded shrinkages greatly exceed calculated shrinkages cannot be attributed to a deficiency in the theoretical expressions customarily invoked. It is explained, instead, by anharmonic effects in bending modes that give the illusion of anomalous shrinkage where it does not, in fact, exist. These effects, which skew the nonbonded distribution functions and displace the true mean distances from the peak maxima, contain heretofore unexploited information about anharmonic potential constants.en_US
dc.format.extent3102 bytes
dc.format.extent308124 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleElectron diffraction studies of hot molecules. II. ‘‘Anharmonic shrinkage effects’’ in SF6, CF4, and SiF4en_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Chemistry, University of Michigan, Ann Arbor, Michigan 48109en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70624/2/JCPSA6-77-4-1874-1.pdf
dc.identifier.doi10.1063/1.444039en_US
dc.identifier.sourceThe Journal of Chemical Physicsen_US
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dc.identifier.citedreferenceIn prior electron diffraction literature the symbol a has been used to represent two different quantities, one a temperature‐independent Morse potential constant and, the other [the a of Eq. (1)], a temperature‐dependent measure of skewness of a distribution function. This has led to so much confusion that we distinguish the latter usage by decorating the symbol with a caret.en_US
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dc.identifier.citedreferenceM. Kelley and M. Fink, Austin Symposium on Molecular Structure, Austin, Texas, March 3, 1980; J. Chem. Phys. (submitted).en_US
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dc.identifier.citedreferenceKelley and Fink also obtained shrinkages which were negative at room temperature. In Fig. 2, a constant amount has been added to their shrinkage at all temperatures to make the room temperature shrinkages agree with the theoretical value at room temperature. Trans shrinkages from their study have not been included in Fig. 1 because uncertainties (comparable to ours) obscured any trend in the range 300—500 K.en_US
dc.identifier.citedreferenceP. M. Morse, Phys. Rev. 34, 57 (1929). For convenient expansions of the ground‐state distribution, see L. S. Bartell, J. Chem. Phys. 23, 1219 (1955); Ref. 7, second citation.en_US
dc.identifier.citedreferenceIn analyses of diffraction data for hot CF3Cl,CF3Cl, where internuclear distances overlap more than they do in the fluorides of this study, Vance has found that asymmetry parameter values for one distance do affect the derivation of other internuclear distances. He has also observed some effect on amplitudes of vibration. L. S. Bartell, W. Vance, and S. R. Goates (unpublished).en_US
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dc.identifier.citedreferenceW. J. Adams, H. B. Thompson, and L. S. Bartell, J. Chem. Phys. 53, 4040 (1970).en_US
dc.owningcollnamePhysics, Department of


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