1972
DOI: 10.1063/1.1678080
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Raman Spectra of Gases. IV. Methylenecyclobutane and Trimethylene Sulfide

Abstract: The low frequency Raman spectra of methylenecyclobutane and trimethylene sulfide in the gaseous state have been recorded. The observed Q branches for the ring puckering vibration have been assigned as Av=2 transitions from a double minimum potential function. The Q branches for trimethylene sulfide agreed with those predicted from far infrared and microwave data and confirm the predicted energy difference for the v=2 to 3 transition. This is the first direct observation of the ring puckering vibration for meth… Show more

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Cited by 40 publications
(11 citation statements)
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“…Experimentally, it was found using mid-IR spectrum, microwave spectrum and Raman spectrum to be 168 AE 10, 160 AE 40 and 141 AE 5 cm À1 , respectively. 16,27,28 Another fundamental ring puckering is located at $ 658 cm À1 , which is in good agreement with the same mode found at 657.2 cm À1 using mid-IR spectrum 16 and con¯rmed by Raman spectrum. 28 The C¼C stretching theoretically located at $ 1770 cm À1 is experimentally observed at 1675 cm À1 (note that the authors did not assign which mode is which).…”
Section: Methylenecyclobutanesupporting
confidence: 75%
See 1 more Smart Citation
“…Experimentally, it was found using mid-IR spectrum, microwave spectrum and Raman spectrum to be 168 AE 10, 160 AE 40 and 141 AE 5 cm À1 , respectively. 16,27,28 Another fundamental ring puckering is located at $ 658 cm À1 , which is in good agreement with the same mode found at 657.2 cm À1 using mid-IR spectrum 16 and con¯rmed by Raman spectrum. 28 The C¼C stretching theoretically located at $ 1770 cm À1 is experimentally observed at 1675 cm À1 (note that the authors did not assign which mode is which).…”
Section: Methylenecyclobutanesupporting
confidence: 75%
“…16,27,28 Another fundamental ring puckering is located at $ 658 cm À1 , which is in good agreement with the same mode found at 657.2 cm À1 using mid-IR spectrum 16 and con¯rmed by Raman spectrum. 28 The C¼C stretching theoretically located at $ 1770 cm À1 is experimentally observed at 1675 cm À1 (note that the authors did not assign which mode is which). 29 The same C¼C stretching mode can be compared with the C¼C stretching mode of 2-methylpropene observed at 1661 cm À1 .…”
Section: Methylenecyclobutanesupporting
confidence: 75%
“…same reasoning as for trimethylene oxide [5] and expect that the Av = 2 transitions (v the puckering quantum number) should appear most prominently in the Raman spectra. In fact this has been observed for normal TMS [2], and it is not surprising to find it also for the deuterated compounds. The line positions are given in the spectra shown in Figures 1 to 5.…”
Section: Resultsmentioning
confidence: 84%
“…Indeed, the Raman observable transitions resulting from the ring puckering of the parent compound, i.e. normal TMS, have been reported already by Durig and his group in 1972 [2]. Since only two-quantum transitions are seen in the Raman spectra one could hope that the missing values for the deuterated materials could be determined in this fashion.…”
Section: Introductionmentioning
confidence: 95%
“…However, Durig et al (7) have examined the Raman spectrum and derived a potential function which also explained the microwave data (4) and infrared combination bands (8).…”
Section: Introductionmentioning
confidence: 99%