2009
DOI: 10.1016/j.molstruc.2008.12.011
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The r0 structural parameters, vibrational spectra, ab initio calculations and barriers to internal rotation and linearity of methylisocyanate

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Cited by 12 publications
(11 citation statements)
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“…It is not new that MIC is amongst the molecules exhibiting a strong resonance between the m CH and 2b CH modes [69]. Moreover, Zhou and Durig have recently reported [35] the positions of all three of the CH 3 stretching modes of MIC to have significant differences in frequencies with the changes of phase (for gaseous, liquid and solid MIC), which does not help in the interpretation of the present matrix-isolation experimental data.…”
Section: Methodsmentioning
confidence: 65%
See 1 more Smart Citation
“…It is not new that MIC is amongst the molecules exhibiting a strong resonance between the m CH and 2b CH modes [69]. Moreover, Zhou and Durig have recently reported [35] the positions of all three of the CH 3 stretching modes of MIC to have significant differences in frequencies with the changes of phase (for gaseous, liquid and solid MIC), which does not help in the interpretation of the present matrix-isolation experimental data.…”
Section: Methodsmentioning
confidence: 65%
“…The structure of MIC, barriers to internal rotation as well as the vibrational spectra of this compound have been the subject of several computational studies [30][31][32][33][34]. Experimental infrared and Raman spectra of gaseous, liquid and solid MIC were also reported [34,35].…”
Section: Introductionmentioning
confidence: 99%
“…Electron diffraction (Eyster et al 1940; Anderson et al 1972), microwave (MW) spectra (Curl et al 1963; Lett & Flygare 1967; Koput 1984; Koput 1986; Kasten et al 1986) and theoretical calculations (Koput 1988; Sullivan et al 1994; Zhou & Durig 2009; Reva et al 2010, Dalbouha et al 2016) indicate that the CH 3 NCO molecule is an asymmetric top with a CNC angle of about 140° and a small barrier (≈ 20-30 cm -1 ) for the torsion of the methyl group. Its large amplitude internal motions (CH 3 torsion and CNC bend) complicate the spectral analysis and although the high accuracy of the available experimental data (Cernicharo et al 2016) has allowed the detection of this molecule in the gas phase of the ISM, an appreciable discrepancy persists in the value of the A rotational constant (Halfen et al 2015; Cernicharo et al 2016; Dalbohua et al 2016).…”
Section: Introductionmentioning
confidence: 99%
“…The substitution of the pseudohalogen NCO and NCS to a hydrocarbon (R) results in a very large CNC(X) angle, [1,2] which may result in a very low wavenumber CNC bend with only a few bound vibrational states with the remaining molecules having essentially free internal rotation, which has been found for CH 3 NCO 1 and CH 3 NCS 2 . However, when these pseudohalogens are substituted on a silane, the question arises whether there is more than one bound state for the SiNC(X) bend or simply a small 'hump' in the potential function governing the SiNC bending mode as the effective structure is a linear heavy atom skeleton.…”
Section: Introductionmentioning
confidence: 86%