2000
DOI: 10.1006/jmsp.2000.8070
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Analysis of the “Unusual” Vibrational Components of Triply Degenerate Vibrational Mode ν6 of Mo(CO)6 Based on the Classical Interpretation of the Effective Rotation–Vibration Hamiltonian

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Cited by 25 publications
(29 citation statements)
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“…The high density of vibrational states, the presence of several hot bands, and the numerous possible anharmonic interactions prevented us from resolving the rotational structure in this part of the spectrum. Table III lists In the following paragraphs we present the first rotational analysis and fit of 7 fundamental bands of adamantane: ν 23 , ν 24 , ν 25 , ν 26 , ν 27 , ν 28 , and ν 30 . For the spectral analysis, it is possible to use the tools that have been developed previously for smaller tetrahedral molecules, importantly CH 4 .…”
Section: Resultsmentioning
confidence: 99%
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“…The high density of vibrational states, the presence of several hot bands, and the numerous possible anharmonic interactions prevented us from resolving the rotational structure in this part of the spectrum. Table III lists In the following paragraphs we present the first rotational analysis and fit of 7 fundamental bands of adamantane: ν 23 , ν 24 , ν 25 , ν 26 , ν 27 , ν 28 , and ν 30 . For the spectral analysis, it is possible to use the tools that have been developed previously for smaller tetrahedral molecules, importantly CH 4 .…”
Section: Resultsmentioning
confidence: 99%
“…The three spectra have been recorded with a spectral resolution of 0.001 cm −1 . All bands except ν 23 and ν 30 have been recorded using a globar continuum source together with an MCT detector and a KBr beamsplitter. In the first spectrum (600-4500 cm −1 ) the gas pressure was set to about 0.05 mbar (in order to optimize the detection of the ν 28 mode) and the acquisition time was about 24 h. In the second spectrum (33-600 cm −1 ) we have made use of the SOLEIL synchrotron FIR radiation extracted by the AILES beamline as the continuum source of the FT interferometer, resulting in a significant improvement of the signal-to-noise ratio in comparison with the globar source.…”
Section: A Experimentsmentioning
confidence: 99%
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“…In the case of the Hamiltonian (11.4) whose vibrational part is quadratic, this approximation matches exactly the extrema of the so-called "rotational energy surfaces" [32,36,35], which are obtained when all rotational operators in H eff are replaced by their quantum analogues. Further examples can be found in [58,13,12].…”
Section: Examplesmentioning
confidence: 99%