1969
DOI: 10.1063/1.1672541
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Translational Frequencies of Molecules in Naphthalene, Durene, and Anthracene Single Crystals at Low Temperatures

Abstract: Among the three translational frequencies of these monoclinic molecular crystals, two are expected when the electric field of the radiation is parallel to the monoclinic b axis, and one when the field is perpendicular to b. The infrared absorption spectra show that the last band is obtained in each case for an electric field parallel to the easy cleavage plane, at 66 cm−1 for naphthalene, 65 cm−1 for durene, 61 cm−1 for anthracene. This polarization is explained for naphthalene in terms of the tensor of polari… Show more

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Cited by 41 publications
(11 citation statements)
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“…(3) The situation represents independent librational motions of each molecular partner in its own sublattice. This describes our sublattice limit where the phonon bands of the two sublattices will be observed at different frequencies.…”
Section: Theoretical Discussion Using a Simple Modelmentioning
confidence: 99%
“…(3) The situation represents independent librational motions of each molecular partner in its own sublattice. This describes our sublattice limit where the phonon bands of the two sublattices will be observed at different frequencies.…”
Section: Theoretical Discussion Using a Simple Modelmentioning
confidence: 99%
“…This broadening is not a result of mixing with translational phonons, as the highest translational phonon frequency is only about 105 cm-I (at liquid nitrogen temperature). 31 The broadening can be partially explained by a calculation based on a moment expansion at the amalgamation limit. 28 According to the result of this calculation, the broadening of different modes in a mixed crystal of fixed composition is proportional to the trap depth and the broadening is largest in a 50% mixture.…”
Section: Methodsmentioning
confidence: 99%
“…Using data for naphthalene [29] (a = 8"235~, b= 6"003A, c= 8"658A, 7 = 122"7~ we have V 0 = 360"2.~ 3. ~ is derived from data given in [-30], and we get ~ = 1"2 x 10 a ms -l. The maximum frequency then becomes ~0,, = 9'5 x 1012s-1 and the corresponding Debye temperature 0,r = 72"6 K. Experimental data for the frequencies of the optical phonons are taken from [31][32][33][34][35]. Because these frequencies are temperature dependent it is not possible to derive one exact value for all temperatures.…”
Section: Parameters Of the Modelmentioning
confidence: 99%