Theoretical NMR nJ(13C,13C) Scalar Couplings as Probes to Study Diamagnetic Ring Currents in Fullerenes
In this work J(13C,13C) coupling constants and the principal components of nuclear magnetic shielding constants in the C60, C70, and C60 ( 6 - ) fullerenes are calculated at the B3LYP/cc-pCVDZ-sd level using optimized B3LYP/cc-pCVDZ geometries. Indirect spin-spin couplings are utilized to study loca...
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Academic Press Inc.
2005
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024 | 7 | |2 scopus |a 2-s2.0-33645881094 | |
040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
100 | 1 | |a Contreras, Rubén Horacio | |
245 | 1 | 0 | |a Theoretical NMR nJ(13C,13C) Scalar Couplings as Probes to Study Diamagnetic Ring Currents in Fullerenes |
260 | |b Academic Press Inc. |c 2005 | ||
270 | 1 | 0 | |m Contreras, R.H.; Department of Physics, FCEyN, University of Buenos Aires, Buenos Aires, Argentina |
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506 | |2 openaire |e Política editorial | ||
520 | 3 | |a In this work J(13C,13C) coupling constants and the principal components of nuclear magnetic shielding constants in the C60, C70, and C60 ( 6 - ) fullerenes are calculated at the B3LYP/cc-pCVDZ-sd level using optimized B3LYP/cc-pCVDZ geometries. Indirect spin-spin couplings are utilized to study local diamagnetic ring currents in fullerenes. In unsaturated carbon containing compounds, the Fermi contact (FC) contribution to long-range nJ(13C,13C) (n>4) coupling constants is mainly transmitted through the mobile π-electronic system following a few simple rules: the alternating sign-rule and the pathway invariance. Besides, the absolute value of such a coupling decreases slowly when increasing the number of bonds separating the coupled nuclei. Without explicitly addressing the controversial topic of the aromaticity of fullerenes, we show that the π-transmitted components of the FC contribution provide information on factors affecting ring currents in fullerenes. © 2005 Elsevier Inc. All rights reserved. |l eng | |
536 | |a Detalles de la financiación: EEC-0118007, NSF-CHE9982156 | ||
536 | |a Detalles de la financiación: Welch Foundation | ||
536 | |a Detalles de la financiación: Intel Corporation | ||
536 | |a Detalles de la financiación: Rice University, EIA-0216467 | ||
536 | |a Detalles de la financiación: Secretaría de Ciencia y Técnica, Universidad de Buenos Aires, X222 | ||
536 | |a Detalles de la financiación: Consejo Nacional de Investigaciones Científicas y Técnicas, PIP 2140 | ||
536 | |a Detalles de la financiación: RHC gratefully acknowledges economic support from UBACyT (X222) and CONICET (PIP 2140). This work was supported by the Nanoscale Science and Engineering Initiative of the National Science Foundation under NSF Award Number EEC-0118007, NSF-CHE9982156. Calculations were performed at the Rice Terascale Cluster funded by NSF under Grant EIA-0216467, Intel, HP, and the Welch Foundation. | ||
593 | |a Department of Physics, FCEyN, University of Buenos Aires, Buenos Aires, Argentina | ||
593 | |a Department of Chemistry, Rice University, Houston, TX 77005-1892, United States | ||
700 | 1 | |a Peralta, J.E. | |
700 | 1 | |a Barone, V. | |
700 | 1 | |a Scuseria, G.E. | |
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