CCSD calculations on C14, C18, and C22 carbon clusters
Author(s) -
Sundaram Arulmozhiraja,
Takahisa Ohno
Publication year - 2008
Publication title -
the journal of chemical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.071
H-Index - 357
eISSN - 1089-7690
pISSN - 0021-9606
DOI - 10.1063/1.2838200
Subject(s) - bond length , ring (chemistry) , cluster (spacecraft) , chemistry , carbon fibers , distortion (music) , crystallography , density functional theory , single bond , molecular geometry , atomic physics , molecular physics , computational chemistry , materials science , molecule , physics , crystal structure , group (periodic table) , organic chemistry , amplifier , optoelectronics , cmos , composite number , computer science , composite material , programming language
The structure and energetics of the ring isomers of C(4n+2) (n=3-5) carbon clusters were studied by using coupled-cluster singles and doubles excitation theory to overcome the vast differences existing in the literature. The results obtained in the present study clearly indicate that C(14), C(18), and C(22) carbon rings have bond-length and bond-angle alternated acetylenic minimum energy structures. Contrarily, density functional theory calculations were unable to predict these acetylenic-type structures and they ended up with the cumulenic structures. It is found from the coupled-cluster studies that the lowest-energy ring isomer for the first two members of C(4n+2) series is a bond-angle alternated cumulenic D((2n+1)h) symmetry structure while the same for the remaining members is a bond-length and bond-angle alternated C((2n+1)h) symmetry structure. In C(4n+2) carbon rings, Peierls-type distortion, transformation from bond-angle alternated to bond-length alternated minimum energy structures, occurs at C(14) carbon ring.
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