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Hindered Rotation in Molecules with Relatively High Potential Barriers

dc.contributor.authorHecht, Karl T.en_US
dc.contributor.authorDennison, David M.en_US
dc.date.accessioned2010-05-06T21:25:32Z
dc.date.available2010-05-06T21:25:32Z
dc.date.issued1957-01en_US
dc.identifier.citationHecht, Karl T.; Dennison, David M. (1957). "Hindered Rotation in Molecules with Relatively High Potential Barriers." The Journal of Chemical Physics 26(1): 31-47. <http://hdl.handle.net/2027.42/69966>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/69966
dc.description.abstractThe theory of hindered rotation has been applied to the type of asymmetric molecule in which the hindering barrier is high enough so that the hindered rotation splittings of the energy levels are small compared with the rotational energies but yet large enough to be observable in the microwave spectrum. The specific type of molecule considered consists of a rigid asymmetric component which may undergo a hindered rotation about the symmetry axis of a rigid symmetric component where the symmetric component is in addition assumed to have threefold symmetry and the asymmetric component at least a plane of symmetry containing the symmetry axis of the symmetric component. An example might be the acetaldehyde molecule, CH3CHO.In principle, the theory developed by Burkhard and Dennison can be used directly but in practice the method is difficult to apply to such a molecule since the matrix elements of the Hamiltonian used previously do not degenerate naturally or easily to those for the rigid asymmetric rotator in the infinite barrier limit. In the present treatment a transformation is made on the Hamiltonian whereby this complication is avoided and the resulting calculations are greatly simplified.It is found that the spectrum is essentially that of the rigid rotator with the important exception that all the strong lines are split into two components. For the low J transitions specific formulas have been derived for these splittings which are relatively simple functions of the barrier height, the principal moments of inertia, and two additional parameters involving the molecular dimensions and the masses. The barrier height can thus be deduced from the observed splittings without the use of the somewhat cumbersome machinery needed in the general case.en_US
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dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleHindered Rotation in Molecules with Relatively High Potential Barriersen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumHarrison M. Randall Laboratory of Physics, University of Michigan, Ann Arbor, Michiganen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/69966/2/JCPSA6-26-1-31-1.pdf
dc.identifier.doi10.1063/1.1743262en_US
dc.identifier.sourceThe Journal of Chemical Physicsen_US
dc.identifier.citedreferenceJ. S. Koehler and D. M. Dennison, Phys. Rev. 57, 1006 (1940).en_US
dc.identifier.citedreferenceD. G. Burkhard and D. M. Dennison, Phys. Rev. 84, 408 (1951).en_US
dc.identifier.citedreferenceE. V. Ivash and D. M. Dennison, J. Chem. Phys. 21, 1804 (1953).en_US
dc.identifier.citedreferenceA generalization to molecules consisting of a completely asymmetric component linked to a symmetric component will be discussed briefly in an appendix. The generalization to molecules in which the symmetric component has k‐fold symmetry, with k>3,k>3, is very straightforward. However, if k  =  2,k=2, the molecule will in general consist of two asymmetric components, and although the methods used can, in principle, be extended to this case also, the theory becomes very complicated due to the complete asymmetry of both components.en_US
dc.identifier.citedreferenceTannenbaum, Johnson, Myers, and Gwinn, J. Chem. Phys. 22, 949 (1954).en_US
dc.identifier.citedreferenceWilson, Lin, and Lide, J. Chem. Phys. 23, 136 (1955).en_US
dc.identifier.citedreferenceH. H. Nielsen, Phys. Rev. 40, 445 (1932).en_US
dc.identifier.citedreferenceThe diagonalization of the matrix elements is easier in this new form even if the barrier to hindered rotation is a relatively low one. The n→n′n→n′ connections (n′ ≠ n)(n′≠n) besides being simpler in form, now give only very small contributions to the energies for any state lying appreciably below the top of the barrier, and even for states lying above the top of the barrier the n→n′n→n′ connections will be smaller than those occurring in the earlier formulation.en_US
dc.identifier.citedreferenceKing, Hainer, and Cross, J. Chem. Phys. 11, 27 (1943).en_US
dc.identifier.citedreferenceH. D. Koenig, Phys. Rev. 44, 657 (1933).en_US
dc.identifier.citedreferenceFor the En,En, see also, Tables Relating to Mathieu Functions (Columbia University Press, New York, 1951), p. XVIII.en_US
dc.identifier.citedreferenceSee, for example, E. B. Wilson and J. B. Howard, J. Chem. Phys. 4, 260 (1936), Eq. (43).en_US
dc.identifier.citedreferenceN. Solimene and B. P. Dailey, J. Chem. Phys. 22, 2042 (1954).en_US
dc.identifier.citedreferenceD. G. Burkhard, Trans. Faraday Soc. 52, 1 (1956).en_US
dc.identifier.citedreferenceD. G. Burkhard, J. Chem. Phys. 21, 1541 (1953); D. G. Burkhard and J. C. Irvin, J. Chem. Phys. 23, 1405 (1955).en_US
dc.owningcollnamePhysics, Department of


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