Shielding-density functions interpret nuclear magnetic shieldings point-wise, through the Biot-Savart law. For aromatic, anti-aromatic, and non-aromatic π-systems (benzene, cyclooctatetraene, borazine), the characteristic pattern of current density leads to a distinctive map for the π-contribution to the perpendicular components of 1H shielding-density. Hence, global and localised currents have distinguishable signatures, dependent on separation between outward and return circulations in the current-density map. Aromatic, diatropic π-current produces an intense deshielding ipso spike, weakly cancelled by a remote shielding ridge; paratropic anti-aromatic π-current inverts these features; localised π-currents produce cancelling shielding/deshielding spikes. Ring-currents also contribute characteristically to out-of-plane carbon shieldings. © 2004 Elsevier B.V. All rights reserved.
Ring-current signatures in shielding-density maps
Soncini A.;
2005
Abstract
Shielding-density functions interpret nuclear magnetic shieldings point-wise, through the Biot-Savart law. For aromatic, anti-aromatic, and non-aromatic π-systems (benzene, cyclooctatetraene, borazine), the characteristic pattern of current density leads to a distinctive map for the π-contribution to the perpendicular components of 1H shielding-density. Hence, global and localised currents have distinguishable signatures, dependent on separation between outward and return circulations in the current-density map. Aromatic, diatropic π-current produces an intense deshielding ipso spike, weakly cancelled by a remote shielding ridge; paratropic anti-aromatic π-current inverts these features; localised π-currents produce cancelling shielding/deshielding spikes. Ring-currents also contribute characteristically to out-of-plane carbon shieldings. © 2004 Elsevier B.V. All rights reserved.Pubblicazioni consigliate
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