Solid-State NMR and Density Functional Investigation of Carbon-13 Shielding Tensors in Metal−Olefin Complexes

We have determined the principal elements of the chemical shift tensors for a series of metal−olefin complexes:  [Ag(cod)2]BF4 (cod = cis,cis-cycloocta-1,5-diene), [CuCl(cod)]2, PtCl2(cod), [RhCl(cod)]2, and K[PtCl3(C2H4)] using magic-angle sample spinning and a Bayesian probability method to deduce...

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Veröffentlicht in:The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Molecules, spectroscopy, kinetics, environment, & general theory, 1997-11, Vol.101 (47), p.8908-8913
Hauptverfasser: Havlin, Robert, McMahon, Michael, Srinivasan, Ranjani, Le, Hongbiao, Oldfield, Eric
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Sprache:eng
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Zusammenfassung:We have determined the principal elements of the chemical shift tensors for a series of metal−olefin complexes:  [Ag(cod)2]BF4 (cod = cis,cis-cycloocta-1,5-diene), [CuCl(cod)]2, PtCl2(cod), [RhCl(cod)]2, and K[PtCl3(C2H4)] using magic-angle sample spinning and a Bayesian probability method to deduce μ, ρ in the Herzfeld-Berger equations. These principal elements have also been computed by using density functional methods with two different types of functionals and partial geometry optimization. The overall slope and R 2 values between the theoretical and experimental tensor elements are good, ranging from 1.06 to 1.16 for the slope (versus the ideal value of 1) and 0.98−0.99 for the goodness of fit parameter R 2 (versus the ideal value of 1). The use of a hybrid functional results in a slightly worse slope, an effect which is largest for the compounds with the largest paramagnetic shifts. There are no particularly good correlations between C−C bond lengths, isotropic/anisotropic shift tensor elements or computed bond orders; however, the correlation between shielding and (Mulliken) charge of ∼ −120 ppm/electron is consistent with previous experimental estimates on olefins and aromatic compounds. The orientations of the shielding tensor elements in the cod complexes change in a relatively continuous manner with increases in shielding (from d10 to d8 metals), with δ33 becoming rotated (37.5°) from the normal to the CC bond axis in [RhCl(cod)]2. Overall, these results indicate that density functional methods permit the relatively accurate reproduction of metal−ligand shielding patterns in systems whose structures are known, which should facilitate their use in probing metal−ligand geometries in systems whose structures are less certain, such as in metalloproteins.
ISSN:1089-5639
1520-5215
DOI:10.1021/jp972058e