Abstract:Pure six-fold symmetry (V 6 ) internal rotation poses significant challenges to experimental and theoretical determination, as the very low torsional barriers result in huge tunneling splittings difficult to identify and to model. Here we resolved the methyl group internal rotation dynamics of 2,6-and 3,5-difluorotoluene using a newly developed computer code especially adapted to V 6 problems. The jet-cooled rotational spectra of the title molecules in the 5-25 GHz region revealed internal rotation tunneling d… Show more
“…It is known that there is a negligible barrier to the internal rotation of CH 3 in toluene 25 while the addition of substituents to the benzene ring introduces an asymmetry into molecular orbitals that leads to an increased barrier. 26–29 The ( V 3 ) barrier to internal rotation of CH 3 has been determined for different structural isomers of methylthiazole, 30–32 methyloxazole 33 and methylimidazole. 9 The magnitude of the parameter depends on the asymmetry of the molecular orbitals with which the CH 3 group interacts.…”
Broadband microwave spectra have been recorded between 7.0 and 18.5 GHz for N-methylimidazole…H2O and 2-methylimidazole…H2O complexes. Each complex was generated by co-expansion of low concentrations of methylimidazole and H2O in...
“…It is known that there is a negligible barrier to the internal rotation of CH 3 in toluene 25 while the addition of substituents to the benzene ring introduces an asymmetry into molecular orbitals that leads to an increased barrier. 26–29 The ( V 3 ) barrier to internal rotation of CH 3 has been determined for different structural isomers of methylthiazole, 30–32 methyloxazole 33 and methylimidazole. 9 The magnitude of the parameter depends on the asymmetry of the molecular orbitals with which the CH 3 group interacts.…”
Broadband microwave spectra have been recorded between 7.0 and 18.5 GHz for N-methylimidazole…H2O and 2-methylimidazole…H2O complexes. Each complex was generated by co-expansion of low concentrations of methylimidazole and H2O in...
“…Only in 2,6-difluorotoluene, the potential is V 6 due to symmetry. [13] As mentioned, the barrier hindering a methyl rotation is quite sensitive to many structural and electronic effects. In a systematic investigation on a series of methyl alkyl ketones, Andresen et al proposed a link between the torsional barrier of the acetyl methyl group and the molecular structure at the other side of the carbonyl bond.…”
“…Especially for spectroscopy, the rotational spectrum of toluene has always attracted attention since its microwave spectrum was recorded and analyzed for the first time by Rudolph et al [1] Not only the structure of toluene was determined to great accuracy, several theoretical models and program codes have been also developed to reproduce the V 6 potential arising from the internal rotation of the C 3v methyl group attached to a phenyl frame with C 2v symmetry. [2][3][4][5] To gain insights into the substitution effect on this large amplitude motion (LAM) of toluene, studies on many fluorinated derivatives have been performed, such as the investigations on three isomers of fluorotoluene, [6][7][8] a systematic microwave investigation on the six isomers of difluorotoluene, [9][10][11][12][13] and the work on two isomers of trifluorotoluene. [14] All these studies have shown a variety of the potentials of the methyl torsion in both shape and height, which depend on the substituted position(s) of the fluorine atom(s).…”
Large amplitude motion of methyl groups in isolated molecules is a fundamental phenomenon in molecular physics. The methyl torsional barrier is sensitive to the steric and electronic environment in the surrounding of the methyl group, making the methyl group a detector of the molecular structure. To probe this effect, the microwave spectrum of 2,6‐dimethylfluorobenzene, one of the six isomers of dimethylfluorobenzene, was measured using two pulsed molecular jet Fourier transform microwave spectrometers operating in the frequency range from 2 to 40 GHz. Due to internal rotations of two equivalent methyl groups with relatively low torsional barriers, all rotational transitions split into quartets with separations of up to several hundreds of MHz. The splittings were analyzed and modeled to deduce a torsional barrier of 236.7922 (21) cm−1. The results are compared to those obtained from quantum chemical calculations and with other fluorine substituted toluene derivatives of the current literature where the methyl group is adjacent to a fluorine atom.
“…An example is seen in the change of the potential barrier of toluene for various levels of halogenation around the benzyl ring. In toluene, the V 6 barrier is reported as 4.837920599(11) cm −1 ,[2] and increases for p-chlorotoluene (4.872(14) cm −1 )[3], 3,5-difluorotoluene (7.156(84) cm −1 )[4] and 2,4-difluorotoluene (12.432(20) cm −1 ), [4] but decreases slightly for p-fluorotoluene (4.8298(64) cm −1 ) [5]. In a more recent study, an investigation of p-halotoluenes found a p-chlorotoluene V 6 barrier of 4.836(29) cm −1 , which was also found to be a good barrier to describe the tunneling motion in p-bromotoluene and p-iodotoluene.…”
The rotational spectrum of 3-methylphenylacetylene has been recorded in the 2-8 GHz region using a broadband chirped-pulse microwave spectrometer. Torsionrotation transition splittings are observed from a tunneling motion along the methyl internal rotation axis. The XIAM program was used to characterize the splitting, yielding an internal rotation barrier, V 3 , of 11.21745 ± 0.00002 cm −1 .While this barrier is considered low, fits of A-state only transitions yield a quality, rigid-rotor fit and are compared to the combined A/E fits. Computationally predicted barriers are estimated between 14.4 and 28.9 cm −1 .
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