2007
DOI: 10.1016/j.ijms.2006.11.005
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Parity alternation of linear ground-state CnS2− (n=6–18) clusters

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Cited by 6 publications
(2 citation statements)
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“…The majority of negative charge is located at the sulfur atom as well as distributed on the two carbon atoms close to the other end. The structure of C n S 2− ( n = 6−18) is stabilized due to obvious reduction of the Coulomb repulsion force . In ground-state CsC n − ( n = 4−10), the large Cs + seems to be lightly embraced by C n 2− , and the structure of the C n frame reflects the geometry of the corresponding carbon dianion.…”
Section: Resultsmentioning
confidence: 99%
“…The majority of negative charge is located at the sulfur atom as well as distributed on the two carbon atoms close to the other end. The structure of C n S 2− ( n = 6−18) is stabilized due to obvious reduction of the Coulomb repulsion force . In ground-state CsC n − ( n = 4−10), the large Cs + seems to be lightly embraced by C n 2− , and the structure of the C n frame reflects the geometry of the corresponding carbon dianion.…”
Section: Resultsmentioning
confidence: 99%
“…The structure of phosphorus clusters in different charge states has been investigated by various quantum chemical methods [15][16][17][18][19][20][21][22][23][24][25][26] ranging from a molecular dynamics/density functional MD/DF approach [15] to coupled-cluster theory CCSD(T) [19] and comprehensive genetic algorithm DFT [26]. Compared to extensive computational studies of neutral phosphorus clusters [16-19, 21, 22, 26], much less is known about charged clusters, which were most frequently investigated experimentally.…”
Section: Introductionmentioning
confidence: 99%