2006
DOI: 10.1016/j.jms.2006.02.013
|View full text |Cite
|
Sign up to set email alerts
|

Gas phase electronic spectrum of propadienylidene C3H2

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

2
31
0

Year Published

2011
2011
2022
2022

Publication Types

Select...
5
2
1

Relationship

2
6

Authors

Journals

citations
Cited by 30 publications
(33 citation statements)
references
References 15 publications
2
31
0
Order By: Relevance
“…The equilibrium geometry of the reference electronic ground state of l-C 3 H 2 is optimized at the Møller-Plesset perturbation level of theory employing second order (MP2) and fourth order (MP4) corrections and also by the B3LYP [32] method using the aug-cc-pVTZ basis set of Dunning [33]. The optimized equilibrium geometry parameters are given in Table 1 along with the available literature data [19,34,35]. It can be seen from the table that the geometry parameters agree well with the literature data.…”
Section: Electronic Ground and Excited States Of L-c 3 Hmentioning
confidence: 99%
See 1 more Smart Citation
“…The equilibrium geometry of the reference electronic ground state of l-C 3 H 2 is optimized at the Møller-Plesset perturbation level of theory employing second order (MP2) and fourth order (MP4) corrections and also by the B3LYP [32] method using the aug-cc-pVTZ basis set of Dunning [33]. The optimized equilibrium geometry parameters are given in Table 1 along with the available literature data [19,34,35]. It can be seen from the table that the geometry parameters agree well with the literature data.…”
Section: Electronic Ground and Excited States Of L-c 3 Hmentioning
confidence: 99%
“…The intense band between $200-300 Å region is attributed to the optically allowed e C 1 A 1 e X 1 A 1 transition in l-C 3 H 2 [6]. The gas phase measurement of the electronic absorption spectrum of l-C 3 H 2 was also attempted by cavity ring-down (CRD) spectroscopy [19]. This experiment was unsuccessful and a life-time of less than a picosecond of the e B state was envisaged for this failure.…”
Section: Introductionmentioning
confidence: 99%
“…[11][12][13][14] Attempts to measure the 1 3 Σ − u ← X 3 Σ − g transition for the smallest members HC 3 H and HC 5 H in the gas phase failed so far. Whereas the two C 3 H 2 isomers with C 2v symmetry, which are more stable, were studied, [15][16][17][18][19] arguments were given for the non-observation of the electronic transition of HC 5 H, including low oscillator strength and unfavorable production conditions. 13 Several low-energy isomers of C 5 H 2 were investigated by quantum chemistry and microwave absorption spectrosa) Electronic mail: m.steglich@web.de b) Electronic mail: j.p.maier@unibas.ch copy.…”
Section: Introductionmentioning
confidence: 99%
“…[17][18][19][22][23][24] In addition to the fundamental chemical physics appeal, this particular band system has also been the source of a great deal of interest in the astrophysical community. As H 2 CCC is the simplest stable 84 cumulene carbene, a class of molecules that were postulated long ago 85 as potential carriers of DIBs, 86 it has attracted wide interest since its discovery in the diffuse interstellar medium.…”
Section: Astrophysical Relevance Of Excited Singlet Statesmentioning
confidence: 99%
“…They observed levels associated with the symmetry-forbiddenà 1 A 2 ←X 1 A 1 transition, but were initially unable to observe the stronger, symmetry-allowed B 1 B 1 ←X 1 A 1 transition because of the short lifetime of thẽ B 1 B 1 state. 22,23 Subsequently, they succeeded in measuring the prominent vibronic features of theB 1 B 1 ←X 1 A 1 transition at 4881 and 5450 Å, thus providing the basis for assigning these features in the DIB spectrum to propadienylidene. 24 Additional discussion of this topic is deferred to Sec.…”
Section: Introductionmentioning
confidence: 99%