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0042100474
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85033182059
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note
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In Ref. 23(c), bands were observed for benzene trimer that had polarization characteristics consistent with their being intermolecular transitions that gain their intensity by something other than the libration-induced mechanism. However, since these bands could not be unambiguously assigned, the source of their Raman intensity could not be unequivocally identified.
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-
-
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32
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85033185286
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note
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The pulsed-valve driver electronics were built based on a design by Professor M. Sulkes, Department of Chemistry, Tulane University.
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-
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33
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0000699607
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The quantity represented by Eq. (1) is similar to the polarization-independent scattering coefficient that is often dealt with in considerations of the Raman activity of a molecular normal mode - e.g., see J. Martin and S. Montero, J. Chem. Phys. 80, 4610 (1984). In the case of Eq. (1), however, the two Raman fields are assumed to have parallel, linear polarizations. Further, the applicability of Eq. (1) requires no assumption about the vibrational states except that vibrational and rotational motions are separable in the species.
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Martin, J.1
Montero, S.2
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35
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0004161642
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For example, see R. N. Zare, Angular Momentum (Wiley, New York, 1988), Chap. 5.
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Zare, R.N.1
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36
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0004003691
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McGraw-Hill, New York, Appendix III
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For example, see E. B. Wilson, Jr., J. C. Decius, and P. C. Cross, Molecular Vibrations (McGraw-Hill, New York, 1955), Appendix III.
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Wilson Jr., E.B.1
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Cross, P.C.3
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85033178075
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-1, from J. O. Hirschfelder, C. F. Curtis, and R. B. Bird, Molecular Theory of Gases and Liquids (Wiley, New York, 1954), p. 950.
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Molecular Theory of Gases and Liquids Wiley, New York
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40
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85033181814
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-
note
-
Aside from the inclusion of the Coriolis term, Eq. (5) differs from Eq. (1) of Ref. 26 only by a θ-independent term in the potential energy. We have written Eq. (5) in this way to be consistent with the notation and conventions of Friedrich and Herschbach (see. e.g., Ref. 25).
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41
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0001726869
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