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The Geometry and Electronic Topology of Higher-Order Charged Möbius Annulenes

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posted on 2009-10-29, 00:00 authored by Chaitanya S. Wannere, Henry S. Rzepa, B. Christopher Rinderspacher, Ankan Paul, Charlotte S. M. Allan, Henry F. Schaefer, Paul v. R. Schleyer
Higher-order aromatic charged Möbius-type annulenes have been <i>L</i><sub>k</sub>realized computationally. These charged species are based on strips with more than one electronic half-twist, as defined by their linking numbers. The B3LYP/6-311+G(d,p) optimized structures and properties of annulene rings with such multiple half-twists (C<sub>12</sub>H<sub>12</sub><sup>2+</sup>, C<sub>12</sub>H<sub>12</sub><sup>2−</sup>, C<sub>14</sub>H<sub>14</sub>, C<sub>18</sub>H<sub>18</sub><sup>2+</sup>, C<sub>18</sub>H<sub>18</sub><sup>2−</sup>, C<sub>21</sub>H<sub>21</sub><sup>+</sup>, C<sub>24</sub>H<sub>24</sub><sup>2−</sup>, C<sub>28</sub>H<sub>28</sub><sup>2+</sup>, and C<sub>28</sub>H<sub>28</sub><sup>2−</sup>) have the nearly equal C−C bond lengths, small dihedral angles around the circuits, stabilization energies, and nucleus-independent chemical shift values associated with aromaticity. The topology and nature of Möbius annulene systems are analyzed in terms of the torus curves defined by electron density functions (ρ(<i>r</i>)<sub>π</sub>, ELF<sub>π</sub>) constructed using only the occupied π-MOs. The π-torus subdivides into a torus knot for annulenes defined by an odd linking number (<i>L</i><sub>k</sub> = 1, 3π) and a torus link for those with an even linking number (<i>L</i><sub>k</sub> = 2, 4π). The torus topology is shown to map onto single canonical π-MOs only for even values of <i>L</i><sub>k</sub>. Incomplete and misleading descriptions of the topology of π-electronic Möbius systems with an odd number of half twists result when only signed orbital diagrams are considered, as is often done for the iconic single half twist system.

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