Research Article
The origin of the two-electron/four-centers C
C bond in π-TCNE22− dimers: Electrostatic or dispersion?
Article first published online: 15 NOV 2006
DOI: 10.1002/jcc.20525
Copyright © 2006 Wiley Periodicals, Inc.
Issue

Journal of Computational Chemistry
Special Issue: “90 Years of Chemical Bonding”
Volume 28, Issue 1, pages 326–334, 15 January 2007
Additional Information
How to Cite
García-Yoldi, I., Mota, F. and Novoa, J. J. (2007), The origin of the two-electron/four-centers C
C bond in π-TCNE22− dimers: Electrostatic or dispersion?. J. Comput. Chem., 28: 326–334. doi: 10.1002/jcc.20525
Publication History
- Issue published online: 1 DEC 2006
- Article first published online: 15 NOV 2006
- Manuscript Accepted: 18 MAY 2006
- Manuscript Revised: 16 MAY 2006
- Manuscript Received: 10 MAY 2006
Funded by
- Spanish Science and Education Ministry. Grant Numbers: BQU2002-04587-C02-02, CTQ2005-02329
- Catalan Autonomous Government. Grant Numbers: 1999SGR-00046, 2005SGR-00036
- Abstract
- Article
- References
- Cited By
Keywords:
- π-TCNE22−dimers;
- two-electron/four-centers C
C bond; - long C
C bonds; - interaction energy;
- HF;
- B3LYP;
- CASSCF;
- MCQDPT calculations
Abstract
The structure and stability of the π-TCNE22− dimers in K2TCNE2 aggregates is revisited trying to find if the origin of their two-electron/four-centers C
C bond are the electrostatic K+-TCNE− interactions or the dispersion interactions between the anions. The study is done at the HF, B3LYP, CASSCF (2,2), and MCQDPT/CASSCF (2,2) levels using the 6-31+G(d) basis set. Our results show that the only minima of this aggregate that preserves the π-TCNE22− structure has the two K+ atoms placed in equatorial positions in between the two TCNE− planes. When the K+ atoms are placed along the D2h axis of the anions the structure is not a minimum. The main energetic component responsible for the stability of these aggregates comes from the cation–anion interactions. However, a proper accounting of the dispersion component (as done in the MCQDPT/CASSCF (2,2) calculations) is needed to make the closed-shell singlet more stable than the open-shell singlet. Thus, the bond results from the combination of the electrostatic and dispersion components, being the first the dominant one. The optimum geometry of the closed-shell singlet is very similar to the experimental one found in crystals. © 2006 Wiley Periodicals, Inc. J Comput Chem 2007

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