2003
DOI: 10.1016/s0301-0104(02)00912-6
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Theoretical modeling of infrared spectra of aspirin and its deuterated derivative

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Cited by 66 publications
(33 citation statements)
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“…Besides, these values are comparable with those found in our recent work dealing with the H/D isotopic effects in H-bond spectra [21]. However, these ratios are different from those used by Blaise et al, [1] and by Boczar et al [22], because in their approaches, low and high-frequency hydrogen stretching vibrations in individual hydrogen bonds are assumed to be harmonic whereas in the present work we use a Morse potential to describe the anharmonicity of the H-bond bridge. Recall that the removal of the harmonic approximation for the slow modes by introducing Morse potential in place of harmonic one has been done by Leviel and Maréchal [23] in a model similar to the present one, involving cyclic dimer, however, without damping.…”
Section: Table Isupporting
confidence: 91%
“…Besides, these values are comparable with those found in our recent work dealing with the H/D isotopic effects in H-bond spectra [21]. However, these ratios are different from those used by Blaise et al, [1] and by Boczar et al [22], because in their approaches, low and high-frequency hydrogen stretching vibrations in individual hydrogen bonds are assumed to be harmonic whereas in the present work we use a Morse potential to describe the anharmonicity of the H-bond bridge. Recall that the removal of the harmonic approximation for the slow modes by introducing Morse potential in place of harmonic one has been done by Leviel and Maréchal [23] in a model similar to the present one, involving cyclic dimer, however, without damping.…”
Section: Table Isupporting
confidence: 91%
“…The corresponding values from X-ray diffraction are also given in the table for comparison. The molecular structure of the 0.975 0.978 C 5 -C 6 -C 7 121.0 120.5 C 6 -C 7 -C 8 -C 9 0.11 0.25 C 2 -C 5 1.519 1.519 C 6 -C 7 -C 8 119.9 119.9 C 7 -C 8 -C 9 -C 10 0.19 0.27 C 5 -C 6 1.401 1.393 C 7 -C 8 -C 9 119.5 119.9 C 8 -C 9 -C 10 -C 5 0.06 0.41 C 6 -C 7 1.395 1.383 C 8 -C 9 -C 10 120.4 120.1 C 9 -C 10 -C 5 -C 6 0.17 0.54 C 7 -C 8 1.394 1.379 C 9 -C 10 -C 5 120.4 120.1 C 2 -C 5 -C 6 -H 6 3.1 6.5 C 8 -C 9 1.395 1.395 C 5 -C 6 -H 6 119.4 119.5 C 5 -C 6 -C 7 -H 7 179.8 172.9 C 9 -C 10 1.394 1.382 C 6 -C 7 -H 7 119.7 117.8 C 6 -C 7 -C 8 -H 9 179.8 176.0 C 10 -C 5 1.402 1.397 C 7 -C 8 -H 9 120.2 121.9 C 7 -C 8 -C 9 -H 9 179.5 177.4 C 6 -H 6 1.088 0.933 C 8 -C 9 -H 10 120.0 126.9 C 8 -C 9 -C 10 -H 10 178.8 177.3 C 7 -H 7 1.086 1.027 C 9 -C 10 -H 11 119.8 115.6 C 8 -H 9 1.086 1.077 C 9 -H 9 1.086 0.956 C 10 -H 10 1.086 0.996 compound with the atom numbering scheme adopted in the computations is shown in Fig. 3.…”
Section: Crystallographic and Molecular Structuresmentioning
confidence: 99%
“…The parameters used in subsequent calculations of the energy splittings have been calculated from the results of the B3LYP/6-311++G** data and are listed in Table 4. The parameter α describing coupling between the O-H stretching mode ν 73 and the mode ν 4 , ν 7 , ν 8 , ν 11 , ν 13 or ν 16 represent an analogue of linear distortion parameters b used for theoretical reproduction of the X-H infrared band shapes of tropolone [34], salicylaldehyde [35] or aspirin [36]. Both different spectroscopic facts thus have the same origin, the anharmonic coupling in the potential energy between the two X-H and X...Y vibrations.…”
Section: Model Calculationsmentioning
confidence: 99%