posted on 2009-10-29, 00:00authored byChaitanya
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.