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On the Theory of Raman Intensities
1.J. H. Van Vleck, Proc. Natl. Acad. Sci. U.S. 15, 754 (1929).
2.G. Placzek, Handbuch der Radiologie, edited by E. Marx (Akademische Verlagsgesellschaft, Leipzig, 1934), Vol. VI, part 2, p. 205.
3.J. Behringer and J. Brandmüller, Z. Elektrochem. 60, 643 (1956).
4.See footnotes 3 and 5 for details and further references.
5.J. Behringer, Z. Elektrochem. 62, 906 (1958).
6.W. Maier and F. Dörr, Appl. Spectroscopy 14, 1 (1960).
7.D. G. Rea, J. Mol. Spectroscopy 4, 499 (1960).
8.A. C. Albrecht, J. Chem. Phys. 33, 156 (1960).
9.See, for example, footnote 3 for details and further references.
10.A discussion and reference to earlier work may be found in footnote 8. [Correction for a sign mistake therein (Eq. 10) is incorporated in the present Eq. (9).]
11.This step already represents a specialization of the formal development given by Van Vleck. However for nonresonance conditions the latter development in effect reduces to this approximation.
12.A subscript ρ in this paper will always refer to an arbitrary molecule fixed coordinate (or corresponding translation). The symbol σ has been similarly used but later will acquire different meanings. Thus whenever reference to two arbitrary coordinates is necessary, the symbols ρ and will be used in cases where confusion might otherwise arise.
13.H. C. Longuet‐Higgins, Proc. Roy. Soc. (London) A235, 537 (1956).
14.J. N. Murrell and J. A. Pople, Proc. Phys. Soc. (London) A69, 245 (1956).
15.C. C. J. Roothaan, Revs. Modern Phys. 23, 69 (1951).
16.T. Yoshino and H. J. Bernstein, Petroleum Institute Conference on Molecular Spectroscopy (Pergamon Press, New York, 1958), p. 141.
17.G. W. Chantry and R. A. Plane, J. Chem. Phys. 32, 319 (1960).
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