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On the Importance of Electron Correlation Effects for the π‐π Interactions in Cyclophanes
Abstract
Correlated ab initio quantum chemical methods based on second‐order perturbation theory and density functional theory (DFT) together with large atomic orbital (AO) basis sets are used to calculate the structures of four cyclophanes with two aromatic rings and one sulphur‐containing phane with one aromatic ring. The calculated geometrical data for [2.2]paracyclophane, cyclophane (superphane), 8,16‐dimethyl[2.2]metacyclophane, 16‐methyl[2.2]metaparacyclophane, and 2,6,15‐trithia[3 4,10][7]metacyclophane are compared to experimental data from X‐ray crystal structure determinations. In all cases, very accurate theoretical predictions are obtained from the recently developed spin‐component‐scaled MP2 (SCS‐MP2) method, in which the deviations are within the experimental accuracy and expected crystal‐packing or vibrational effects. Especially the inter‐ring distances, which are determined by a detailed balance between attractive van der Waals (dispersive) and repulsive (Pauli) contributions, are very sensitive to the level of theory employed. While standard MP2 theory in general overestimates the dispersive interactions (π–π correlations) between the two aromatic rings leading to too short distances (between 3 and 8 pm), the opposite is observed for DFT methods (errors up to 15 pm). This indicates that an explicit account of dispersive‐type electron correlation effects between the clamped aromatic units is essential for a quantitative description of cyclophane structures. In order to distinguish these effects from “normal” van der Waals interactions, the term “overlap‐dispersive” interaction may be employed. The popular B3 LYP hybrid density functional offers no advantage over the pure PBE functional that at least qualitatively accounts for some of the dispersive effects. The use of properly polarized AO basis sets of at least valence‐triple‐ζ quality is strongly recommended to obtain quantitative predictions with traditional wave function methods.
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Cites
Mathews, D. H., Sabina, J., Zuker, M., & Turner, D. H. (1999) · Journal of Molecular Biology · doi:10.1006/jmbi.1999.2700 · Cited by 3,795
Molecular Electronic‐Structure Theory
Helgaker, T., Jørgensen, P., & Olsen, J. (2000) · doi:10.1002/9781119019572 · Cited by 2,594
Cited by
Grimme, S., Antony, J., Ehrlich, S., & Krieg, H. (2010) · The Journal of Chemical Physics · doi:10.1063/1.3382344 · Cited by 59,686
Self-citationSemiempirical GGA‐type density functional constructed with a long‐range dispersion correction
Grimme, S. (2006) · Journal of Computational Chemistry · doi:10.1002/jcc.20495 · Cited by 31,038
Self-citationEffect of the damping function in dispersion corrected density functional theory
Grimme, S., Ehrlich, S., & Goerigk, L. (2011) · Journal of Computational Chemistry · doi:10.1002/jcc.21759 · Cited by 28,221
Self-citationSemiempirical hybrid density functional with perturbative second-order correlation
Grimme, S. (2006) · The Journal of Chemical Physics · doi:10.1063/1.2148954 · Cited by 3,385
Self-citationRiley, K. E., Pitoňák, M., Jurečka, P., & Hobza, P. (2010) · Chemical Reviews · doi:10.1021/cr1000173 · Cited by 759
Metadata
- Authors
- Grimme, S.
- Venue
- Chemistry – A European Journal
- Publisher
- Wiley
- Published
- 2004-07-08
- Volume
- 10
- Issue
- 14
- Pages
- 3423-3429
- ISSN
- 0947-6539 (ISSN-L)
- 1521-3765
- OpenAlex
- W2028993363
- Cited by
- 168
- References
- 2
- FWCI
- 5.73
- Type
- journal article
- Language
- en
- Open access
- closed
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