2001
DOI: 10.1063/1.1361254
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The A 3Σ−–X 3Σ− electronic transition of HC6N

Abstract: A combined matrix and gas phase study is presented to identify the A 3 ⌺ Ϫ -X 3 ⌺ Ϫ electronic transition of the linear triplet isomer of HC 6 N and isotopic derivative DC 6 N. Absorption spectra have been observed in a 6 K neon matrix after mass selective deposition and in the gas phase by cavity ring down spectroscopy through a supersonic planar plasma. The band origin of the 0 0 0 A 3 ⌺ Ϫ -X 3 ⌺ Ϫ electronic transition of HC 6 N is determined to be at 21 208.60͑5͒ cm Ϫ1 , shifted ϳ30 cm Ϫ1 to the blue of th… Show more

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Cited by 14 publications
(11 citation statements)
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“…The observed spectrum resembles that of the iso-electronic cyanopolyyne HC 6 N [14] and dicyanopolyyne, C 5 N 2 [20]. Both these molecules have been studied previously in a similar way, also combining cavity ring-down spectroscopy and supersonic planar plasma expansions.…”
Section: Resultsmentioning
confidence: 57%
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“…The observed spectrum resembles that of the iso-electronic cyanopolyyne HC 6 N [14] and dicyanopolyyne, C 5 N 2 [20]. Both these molecules have been studied previously in a similar way, also combining cavity ring-down spectroscopy and supersonic planar plasma expansions.…”
Section: Resultsmentioning
confidence: 57%
“…The (fitted) band origin is located at 19817.892(1) cm À1 , which is about 0.1 cm À1 (0.03 cm À1 ) red shifted from the value reported in Ref. [13] ( [14]). This is well within the reported uncertainties with which the absolute frequencies could be determined.…”
Section: Resultsmentioning
confidence: 89%
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