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Anomalous intensities and vibrational structure in the absorption spectra of benzene and benzene- d6
The A 1B 2u ← X 1A 1g absorption spectra of benzene are characterized by long progressions in the ring breathing vibration ν 1. For benzene- d 6, in contrast to benzene- h 6, increasing quanta of ν 1 are associated with a proliferation of bands. A model is proposed which incorporates anharmonic coup...
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Published in: | Chemical physics 1992-12, Vol.168 (2), p.211-223 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The
A
1B
2u ←
X
1A
1g absorption spectra of benzene are characterized by long progressions in the ring breathing vibration ν
1. For benzene-
d
6, in contrast to benzene-
h
6, increasing quanta of ν
1 are associated with a proliferation of bands. A model is proposed which incorporates anharmonic coupling between ν
1 and 2ν
10 in the excited state in addition to the anharmonic coupling of different angular momentum components of 6
n
10
2
m
(
n, m = 1, 2), as an explanation of this phenomenon. Two parameters, namely the two anharmonic coupling strengths, and the zero-order frequency differences between ν
1 and 2ν
10 for the two benzene isotopes, are used to achieve excellent agreement between the calculated and measured transition intensities and frequencies for the bands groups 1
n
06
1
0, 1
n
06
0
1 and 1
n
06
2
1 (
n = 1, 2). For benzene-
d
6 the coupling 6.7 cm
−1 for the ν
1…2ν
10, and ν
6[+] + 2 ν
10[−2]…ν
6[−] + 2ν
10[+2] interactions respectively, and the zero-order frequency difference was taken as 20 cm
−1. The corresponding couplings for benzene-
h
6, derived from those of benzene-
d
6, were 17.2 and 9 cm
−1 respectively, and the frequency difference was taken as 238 cm
−1. |
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ISSN: | 0301-0104 |
DOI: | 10.1016/0301-0104(92)87156-4 |